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rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00703.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00702.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00701.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00693.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00692.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00690.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00688.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00686.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00685.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00684.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00683.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00682.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00681.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00679.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00673.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00677.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00670.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00678.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00672.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00669.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00674.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12089"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12038"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12064"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12069"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12033"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12034"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12052"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12040"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12045"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12037"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12036"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12030"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12051"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12039"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02751.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02752.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02754.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02755.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02756.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02758.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02760.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02761.x"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02811.x"/></rdf:Seq></items></channel><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12054" xmlns="http://purl.org/rss/1.0/"><title>Effect of La2O3 Addition on Copper-Nickel Manganese Thermistors for Low-Temperature Applications</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12054</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of La2O3 Addition on Copper-Nickel Manganese Thermistors for Low-Temperature Applications</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jincheng Yao, Junhua Wang, Qing Zhao, Aimin Chang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-06-14T11:20:27.234198-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12054</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12054</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12054</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The introduction of La<sub>2</sub>O<sub>3</sub> to Mn<sub>0.75</sub>Ni<sub>1.25</sub>CuO<sub>4</sub> ceramics was studied on the microstructure and electrical properties. The sintered Mn<sub>0.75</sub>Ni<sub>1.25</sub>CuO<sub>4</sub>-xLa<sub>2</sub>O<sub>3</sub> (0 ≤ <em>x</em> ≤ 0.3) bodies was typical polycrystalline, with cubic spinel structure of copper manganese oxide, rocksalt structure of nickel copper oxide, along with monoclinic phase of copper oxide and orthorhombic perovskite structure of lanthanum manganese oxide. It is found that La doping reduces the material grain size and changes its morphology from the plate-like form to a spherical staking-like form. The shape and size of the grains are strongly influenced by the addition of La to the system. The X-ray photoelectron spectroscopy analysis corroborates the presence of nonequivalent ions at octahedral sites. The obtained ρ<sub>77K</sub>, B<sub>77K/90K</sub> constant and activation energy of the negative temperature coefficient (NTC) Mn<sub>0.75</sub>Ni<sub>1.25</sub>CuO<sub>4</sub>-xLa<sub>2</sub>O<sub>3</sub> thermistors were in the range of 13.19–30.39 Ω cm, 315–326 K, and 0.0272–0.0281 eV, respectively. This means that the electrical properties can be adjusted to desired values, depending on the La content. Such ceramics could be used as potential candidates for NTC thermistors in a temperature range from 20 K to 90K. So these prepared NTC thermistors were intended to be used under low-temperature conditions.</p></div>
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The introduction of La2O3 to Mn0.75Ni1.25CuO4 ceramics was studied on the microstructure and electrical properties. The sintered Mn0.75Ni1.25CuO4-xLa2O3 (0 ≤ x ≤ 0.3) bodies was typical polycrystalline, with cubic spinel structure of copper manganese oxide, rocksalt structure of nickel copper oxide, along with monoclinic phase of copper oxide and orthorhombic perovskite structure of lanthanum manganese oxide. It is found that La doping reduces the material grain size and changes its morphology from the plate-like form to a spherical staking-like form. The shape and size of the grains are strongly influenced by the addition of La to the system. The X-ray photoelectron spectroscopy analysis corroborates the presence of nonequivalent ions at octahedral sites. The obtained ρ77K, B77K/90K constant and activation energy of the negative temperature coefficient (NTC) Mn0.75Ni1.25CuO4-xLa2O3 thermistors were in the range of 13.19–30.39 Ω cm, 315–326 K, and 0.0272–0.0281 eV, respectively. This means that the electrical properties can be adjusted to desired values, depending on the La content. Such ceramics could be used as potential candidates for NTC thermistors in a temperature range from 20 K to 90K. So these prepared NTC thermistors were intended to be used under low-temperature conditions.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12122" xmlns="http://purl.org/rss/1.0/"><title>Investigation of Glaze Layer Formation on Green Ceramic Bodies</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12122</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Investigation of Glaze Layer Formation on Green Ceramic Bodies</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Undine Fischer,, Humberto Chaves, Christos G. Aneziris, Gert Schmidt</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-06-10T12:01:25.966571-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12122</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12122</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12122</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Using a high-speed and high-resolution-camera system of droplets in glaze sprays and their impact on the surface of a green ceramic body based on silicate tiles have been characterized. The influence of the surface tension of the glaze slips on the droplet size distribution and their wetting behavior on contact with the green silicate body surface have been investigated. The unfired glaze layers have been studied by means of scanning electron microscopy and computer tomography. The impact angle of the droplets as well as the size of the droplets is of great importance for a high glaze surface quality.</p></div>
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Using a high-speed and high-resolution-camera system of droplets in glaze sprays and their impact on the surface of a green ceramic body based on silicate tiles have been characterized. The influence of the surface tension of the glaze slips on the droplet size distribution and their wetting behavior on contact with the green silicate body surface have been investigated. The unfired glaze layers have been studied by means of scanning electron microscopy and computer tomography. The impact angle of the droplets as well as the size of the droplets is of great importance for a high glaze surface quality.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12120" xmlns="http://purl.org/rss/1.0/"><title>Aqueous Gelcasting and Pressureless Sintering of Zirconium Diboride Ceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12120</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Aqueous Gelcasting and Pressureless Sintering of Zirconium Diboride Ceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jie Yin, Zhaoquan Zhang, Zhengren Huang, Hui Zhang, Yongjie Yan, Xuejian Liu, Yan Liu, Dongliang Jiang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-06-10T12:01:14.322663-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12120</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12120</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12120</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Dense (97.3%) zirconium diboride (ZrB<sub>2</sub>) ceramics were obtained via gelcasting and pressureless sintering. Four wt% B<sub>4</sub>C was used as sintering aid. ZrB<sub>2</sub>, SiC, and B<sub>4</sub>C can codisperse well in the alkaline region, using a polyacrylate dispersant. Compared with monolithic ZrB<sub>2</sub> (Z), the mechanical properties of ZrB<sub>2</sub>-SiC (ZS) were enhanced. The Vickers hardness and fracture toughness of ZS were (13.1 ± 0.6) GPa and (2.5 ± 0.4) MPa m<sup>1/2</sup>, respectively.</p></div>
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Dense (97.3%) zirconium diboride (ZrB2) ceramics were obtained via gelcasting and pressureless sintering. Four wt% B4C was used as sintering aid. ZrB2, SiC, and B4C can codisperse well in the alkaline region, using a polyacrylate dispersant. Compared with monolithic ZrB2 (Z), the mechanical properties of ZrB2-SiC (ZS) were enhanced. The Vickers hardness and fracture toughness of ZS were (13.1 ± 0.6) GPa and (2.5 ± 0.4) MPa m1/2, respectively.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12123" xmlns="http://purl.org/rss/1.0/"><title>Integration of High-Conductivity Graphite Foam to Metallic Systems Using Ag-Cu-Ti and Ag-Cu-Pd Braze Alloys</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12123</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Integration of High-Conductivity Graphite Foam to Metallic Systems Using Ag-Cu-Ti and Ag-Cu-Pd Braze Alloys</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mrityunjay Singh, Craig Smith, Rajiv Asthana, Andrew Gyekenyesi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-06-06T10:29:34.230198-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12123</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12123</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12123</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Graphite foams with low, medium, and high densities were joined to Cu-clad-Mo, 430 stainless steel, titanium, and Inconel 625 using Cusil-ABA<sup>®</sup> and Palcusil-5<sup>®</sup>. Copper-clad-molybdenum and steel were also joined to SiC-coated foam. Well-bonded joints with partially infiltrated foam and with carbon ligaments enriched with Ti formed in Cusil-ABA joints of coated and uncoated foam. Low-density foams showed greatest braze penetration and penetration distance decreased with increasing foam density. Foam/metal joints with Palcusil-5 showed less penetration than Cusil-ABA. The tension test on foam/Cu-clad-Mo and foam/430 stainless steel joints made using Cusil-ABA revealed that the joints were always stronger than the foam.</p></div>
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Graphite foams with low, medium, and high densities were joined to Cu-clad-Mo, 430 stainless steel, titanium, and Inconel 625 using Cusil-ABA® and Palcusil-5®. Copper-clad-molybdenum and steel were also joined to SiC-coated foam. Well-bonded joints with partially infiltrated foam and with carbon ligaments enriched with Ti formed in Cusil-ABA joints of coated and uncoated foam. Low-density foams showed greatest braze penetration and penetration distance decreased with increasing foam density. Foam/metal joints with Palcusil-5 showed less penetration than Cusil-ABA. The tension test on foam/Cu-clad-Mo and foam/430 stainless steel joints made using Cusil-ABA revealed that the joints were always stronger than the foam.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12048" xmlns="http://purl.org/rss/1.0/"><title>In Situ Synthesis of Nanostructured WC-Co Within Silica Gel Matrix</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12048</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">In Situ Synthesis of Nanostructured WC-Co Within Silica Gel Matrix</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Arpita Dalapati Thakur, Mahua Ghosh Chaudhuri, Gopes C. Das, Rajib Dey, Manoj K. Mitra, Siddhartha Mukherjee</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-06-06T10:27:57.410019-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12048</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12048</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12048</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p><em>In situ</em> reduction of tungstic acid and cobalt chloride by dextrose in silica gel resulted in co-deposition of tungsten carbide-cobalt (WC–Co) nanoparticles with different proportions of cobalt (5–15 wt % of WC). X-ray powder diffraction (XRD), high-resolution transmission electron microscopy (HRTEM), scanning electron microscopy (SEM) and Fourier-transform infrared (FT-IR) spectroscopy have been used for characterizing these nanoparticles. WC-Co aggregates of 25–30 nm size have been achieved, successfully.</p></div>
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In situ reduction of tungstic acid and cobalt chloride by dextrose in silica gel resulted in co-deposition of tungsten carbide-cobalt (WC–Co) nanoparticles with different proportions of cobalt (5–15 wt % of WC). X-ray powder diffraction (XRD), high-resolution transmission electron microscopy (HRTEM), scanning electron microscopy (SEM) and Fourier-transform infrared (FT-IR) spectroscopy have been used for characterizing these nanoparticles. WC-Co aggregates of 25–30 nm size have been achieved, successfully.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12124" xmlns="http://purl.org/rss/1.0/"><title>Electrochemical Deposition of 58SiO2-33CaO-9P2O5 Nanobioactive Glass Particles on Ti-6Al-4V Alloy for Biomedical Applications</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12124</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Electrochemical Deposition of 58SiO2-33CaO-9P2O5 Nanobioactive Glass Particles on Ti-6Al-4V Alloy for Biomedical Applications</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Balasubramaniam Saravanakumar, Muthusamy Prabhu, Venkatachalam Rajendran, Judy Gopal, Uthandi Kamachi Mudali</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-31T09:45:00.298959-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12124</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12124</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12124</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The nanobioactive glass (58SiO<sub>2</sub>-33CaO-9P<sub>2</sub>O<sub>5</sub>) powders were synthesized by simple sol–gel method. The prepared samples reveal amorphous nature, agglomerated spherical morphology with particle size of 100–150 nm. The specific surface area of nanobioactive glass (NBG) particle is 147 m<sup>2</sup>/g. The NBG samples were coated on titanium (Ti-6Al-4V) alloy through electrochemical deposition method. The particle size of the NBG-coated surface was in the order of 200–300 nm, and it was confirmed by atomic force microscopy (AFM) analysis. <em>In vitro</em> and AFM studies reveal the existence of higher bioactivity and uniform coating of NBG on implants at 80 V for 1 h.</p></div>
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The nanobioactive glass (58SiO2-33CaO-9P2O5) powders were synthesized by simple sol–gel method. The prepared samples reveal amorphous nature, agglomerated spherical morphology with particle size of 100–150 nm. The specific surface area of nanobioactive glass (NBG) particle is 147 m2/g. The NBG samples were coated on titanium (Ti-6Al-4V) alloy through electrochemical deposition method. The particle size of the NBG-coated surface was in the order of 200–300 nm, and it was confirmed by atomic force microscopy (AFM) analysis. In vitro and AFM studies reveal the existence of higher bioactivity and uniform coating of NBG on implants at 80 V for 1 h.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12125" xmlns="http://purl.org/rss/1.0/"><title>Synthesis and Photoluminescence Characteristics of YAl3(BO3)4:Tb3+ Phosphors by Combustion Process</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12125</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Synthesis and Photoluminescence Characteristics of YAl3(BO3)4:Tb3+ Phosphors by Combustion Process</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Guifang Li, Zhimin Li, Quanxi Cao, Yunxia Huang, Junyan Shi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-30T10:26:08.879013-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12125</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12125</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12125</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Terbium-activated YAl<sub>3</sub>(BO<sub>3</sub>)<sub>4</sub> (YAl<sub>3</sub>(BO<sub>3</sub>)<sub>4</sub>:Tb<sup>3+</sup>) phosphors were synthesized by both combustion method and solid-state reaction. It was found that the pure-phase YAl<sub>3</sub>(BO<sub>3</sub>)<sub>4</sub> phosphors synthesized by combustion method were obtained at 1000°C, which was 200°C lower than that by solid-state reaction. The average particle size of the combustion-derived phosphors increased with increasing temperatures. The luminescence characteristics in ultraviolet (UV) — vacuum ultraviolet (VUV) ranges for the YAl<sub>3</sub>(BO<sub>3</sub>)<sub>4</sub>:Tb<sup>3+</sup> phosphors were investigated. The bands from 175 nm to 300 nm were attributed to the 4f<sup>8</sup>-4f<sup>7</sup>5d<sup>1</sup> transitions of Tb<sup>3+</sup>. The other strong bands in the region from 125 nm to 175 nm were assigned to host absorption. The emission spectra showed the strongest emission at 542 nm corresponding to the <sup>5</sup>D<sub>4</sub>→<sup>7</sup>F<sub>5</sub> transition of Tb<sup>3+</sup>. Moreover, the combustion-derived YAl<sub>3</sub>(BO<sub>3</sub>)<sub>4</sub>:Tb<sup>3+</sup> phosphors generated more intense luminescence than the solid-state-derived phosphors under UV excitation.</p></div>
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Terbium-activated YAl3(BO3)4 (YAl3(BO3)4:Tb3+) phosphors were synthesized by both combustion method and solid-state reaction. It was found that the pure-phase YAl3(BO3)4 phosphors synthesized by combustion method were obtained at 1000°C, which was 200°C lower than that by solid-state reaction. The average particle size of the combustion-derived phosphors increased with increasing temperatures. The luminescence characteristics in ultraviolet (UV) — vacuum ultraviolet (VUV) ranges for the YAl3(BO3)4:Tb3+ phosphors were investigated. The bands from 175 nm to 300 nm were attributed to the 4f8-4f75d1 transitions of Tb3+. The other strong bands in the region from 125 nm to 175 nm were assigned to host absorption. The emission spectra showed the strongest emission at 542 nm corresponding to the 5D4→7F5 transition of Tb3+. Moreover, the combustion-derived YAl3(BO3)4:Tb3+ phosphors generated more intense luminescence than the solid-state-derived phosphors under UV excitation.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12047" xmlns="http://purl.org/rss/1.0/"><title>A New and Economic Approach to Synthesize and Fabricate Bioactive Diopside Ceramics Using a Modified Domestic Microwave Oven. Part 1: Study of Sintering and Bioactivity</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12047</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A New and Economic Approach to Synthesize and Fabricate Bioactive Diopside Ceramics Using a Modified Domestic Microwave Oven. Part 1: Study of Sintering and Bioactivity</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Abdelhamid Harabi, Souheila Zouai</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-29T11:01:32.356865-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12047</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12047</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12047</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Diopside (CaMgSi<sub>2</sub>O<sub>6</sub>) ceramics was synthesized and fabricated by a simple solid-state reaction rather than other used processes. This new and economic approach for diopside fabrication consists mainly of replacing the usually used starting materials by other more economic (activated CaO·MgO powders), using conventional sintering and microwave sintering. The P<sub>2</sub>O<sub>5</sub> addition (0.5–5.0 wt%) promotes sintering, crystallization, and bioactivity. Additionally, a considerably low weight loss ratio (0.21%) was also obtained for these samples, after 2 days of soaking in lactic acid. Carbonated hydroxyapatite (CHA) formation in simulated body fluid was confirmed for all sintered samples. Both sintering and CHA formation mechanisms were proposed.</p></div>
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Diopside (CaMgSi2O6) ceramics was synthesized and fabricated by a simple solid-state reaction rather than other used processes. This new and economic approach for diopside fabrication consists mainly of replacing the usually used starting materials by other more economic (activated CaO·MgO powders), using conventional sintering and microwave sintering. The P2O5 addition (0.5–5.0 wt%) promotes sintering, crystallization, and bioactivity. Additionally, a considerably low weight loss ratio (0.21%) was also obtained for these samples, after 2 days of soaking in lactic acid. Carbonated hydroxyapatite (CHA) formation in simulated body fluid was confirmed for all sintered samples. Both sintering and CHA formation mechanisms were proposed.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12077" xmlns="http://purl.org/rss/1.0/"><title>Application of Taguchi Method for Characterization of Corrosion Behavior of TiO2 Coating Prepared by Sol-Gel Dipping Technique</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12077</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Application of Taguchi Method for Characterization of Corrosion Behavior of TiO2 Coating Prepared by Sol-Gel Dipping Technique</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sanaz Naghibi, Amin Jamshidi, Omid Torabi, Reza E. Kahrizsangi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-28T10:21:50.604857-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12077</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12077</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12077</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Titanium oxide (TiO<sub>2</sub>) nanoparticle coatings were deposited on the 316L stainless steel substrates by sol-gel method. The morphology, structure, and corrosion resistance of the coating were analyzed using SEM, AFM, X-ray diffraction, and electrochemical techniques. The deposition parameters employed to realize the anticorrosion performance including calcinations temperature, polyethylene glycol (PEG) content, pH value, and number of dipping cycles were investigated. Taguchi statistical experiments were carried out to determine the influence of the deposition variables on anticorrosion properties and optimal conditions. The results indicated that a higher anticorrosion performance of TiO<sub>2</sub> films could be achieved using 1 g of PEG in a sol with pH in range of 7–9, six cycles of dipping, and calcination temperature at 400°C. The Tafel polarization measurements indicate that <em>i</em><sub>corr</sub> value decreases about 200 times and the <em>R</em><sub>corr</sub> value increases around 57 times compared with uncoated 316L stainless steel.</p></div>
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Titanium oxide (TiO2) nanoparticle coatings were deposited on the 316L stainless steel substrates by sol-gel method. The morphology, structure, and corrosion resistance of the coating were analyzed using SEM, AFM, X-ray diffraction, and electrochemical techniques. The deposition parameters employed to realize the anticorrosion performance including calcinations temperature, polyethylene glycol (PEG) content, pH value, and number of dipping cycles were investigated. Taguchi statistical experiments were carried out to determine the influence of the deposition variables on anticorrosion properties and optimal conditions. The results indicated that a higher anticorrosion performance of TiO2 films could be achieved using 1 g of PEG in a sol with pH in range of 7–9, six cycles of dipping, and calcination temperature at 400°C. The Tafel polarization measurements indicate that icorr value decreases about 200 times and the Rcorr value increases around 57 times compared with uncoated 316L stainless steel.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12078" xmlns="http://purl.org/rss/1.0/"><title>Estimation of Activation Energies for Sintering 8 mol % Yttria-Zirconia Using Conventional and Microwave Heating</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12078</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Estimation of Activation Energies for Sintering 8 mol % Yttria-Zirconia Using Conventional and Microwave Heating</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Raghunath R. Thridandapani, Diane C. Folz, David E. Clark</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-28T10:21:24.893877-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12078</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12078</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12078</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The activation energies were estimated for conventional and microwave sintering of Zirconia-8 mol% Yttria (8YZ). The results were analyzed to explain the mechanisms responsible for enhancing flux/mass transport during microwave sintering. The activation energies were evaluated using isothermal and nonisothermal methods. The nonisothermal sintering resulted in higher values of activation energies, as compared to isothermal methods. This behavior may be due to the presence of more than one type of diffusion mechanism dominating throughout the process. The nonisothermal method represented activation energy values close to a single densification mechanism (either volume or grain boundary diffusion). A value of 500 ± 25 kJ/mol was observed for nonisothermal sintering of 8YZ with conventional heating. This value was close to the volume diffusion of Zr<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1111/ijac.12078/asset/equation/ijac12078-math-0001.gif?v=1&amp;t=hi4mvwcf&amp;s=4c587e4f5d02d70c8531774e2b01422aaf1a3841" class="inlineGraphic"/> ion (500 kJ/mol). The microwave sintering (using nonisothermal method) resulted in activation energy values of 200 ± 27 kJ/mol, a value close to the grain boundary diffusion of the Zr<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1111/ijac.12078/asset/equation/ijac12078-math-0002.gif?v=1&amp;t=hi4mvwcg&amp;s=cd0f0cd4683f9da25f0beb013c486db9ffd5f899" class="inlineGraphic"/> ion.</p></div>
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The activation energies were estimated for conventional and microwave sintering of Zirconia-8 mol% Yttria (8YZ). The results were analyzed to explain the mechanisms responsible for enhancing flux/mass transport during microwave sintering. The activation energies were evaluated using isothermal and nonisothermal methods. The nonisothermal sintering resulted in higher values of activation energies, as compared to isothermal methods. This behavior may be due to the presence of more than one type of diffusion mechanism dominating throughout the process. The nonisothermal method represented activation energy values close to a single densification mechanism (either volume or grain boundary diffusion). A value of 500 ± 25 kJ/mol was observed for nonisothermal sintering of 8YZ with conventional heating. This value was close to the volume diffusion of Zr+4 ion (500 kJ/mol). The microwave sintering (using nonisothermal method) resulted in activation energy values of 200 ± 27 kJ/mol, a value close to the grain boundary diffusion of the Zr+4 ion.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12127" xmlns="http://purl.org/rss/1.0/"><title>Silicon Carbide Whisker-Reinforced Ceramic Tape for High-Power Components</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12127</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Silicon Carbide Whisker-Reinforced Ceramic Tape for High-Power Components</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sae Han Na Doo, Won Bae Lim, Jun Seok Lee, Chan Su Han, Yong Soo Cho, Chang Geun Yoo</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-28T10:20:50.50266-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12127</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12127</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12127</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>An attempt to enhance both mechanical strength and thermal conductivity of glass-based tapes is described. Flexural strength of ~420 MPa and thermal conductivity of ~10.3 W/m/K have been achieved in fully densified tape comprising calcium aluminoborosilicate glass, aluminum nitride, and silicon carbide whiskers. Silicon carbide whiskers aligned parallel to the casting direction contributed significantly to the reinforcement of the microstructure with accompanying extensive densification over a broad temperature range. These results are compared with the more typical alumina filler substituted for the aluminum nitride.</p></div>
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An attempt to enhance both mechanical strength and thermal conductivity of glass-based tapes is described. Flexural strength of ~420 MPa and thermal conductivity of ~10.3 W/m/K have been achieved in fully densified tape comprising calcium aluminoborosilicate glass, aluminum nitride, and silicon carbide whiskers. Silicon carbide whiskers aligned parallel to the casting direction contributed significantly to the reinforcement of the microstructure with accompanying extensive densification over a broad temperature range. These results are compared with the more typical alumina filler substituted for the aluminum nitride.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12108" xmlns="http://purl.org/rss/1.0/"><title>Precursor Selection for Sol-Gel Synthesis of Titanium Carbide Nanopowders by a New Intuitionistic Fuzzy Multi-Attribute Group Decision-Making Model</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12108</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Precursor Selection for Sol-Gel Synthesis of Titanium Carbide Nanopowders by a New Intuitionistic Fuzzy Multi-Attribute Group Decision-Making Model</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Fatemeh Hosseinzadeh, Hossein Sarpoolaki, Hassan Hashemi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-28T10:20:37.086067-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12108</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12108</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12108</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>This article develops a new intuitionistic fuzzy multi-attribute group decision-making model to solve precursor selection problems. The proposed model is based on a hybridization of intuitionistic fuzzy sets theory, grey relational analysis and technique for order performance by similarity to ideal solution method. To better describe the uncertain decision environment, multi-attribute group decision-making method with completely unknown weights of both experts and attributes is proposed in an intuitionistic fuzzy setting. Finally, the selection of the carbon source in synthesis of nanocrystalline titanium carbide powders by sol-gel route as an application example is solved by the proposed model, and the implementation of the model is illustrated completely.</p></div>
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This article develops a new intuitionistic fuzzy multi-attribute group decision-making model to solve precursor selection problems. The proposed model is based on a hybridization of intuitionistic fuzzy sets theory, grey relational analysis and technique for order performance by similarity to ideal solution method. To better describe the uncertain decision environment, multi-attribute group decision-making method with completely unknown weights of both experts and attributes is proposed in an intuitionistic fuzzy setting. Finally, the selection of the carbon source in synthesis of nanocrystalline titanium carbide powders by sol-gel route as an application example is solved by the proposed model, and the implementation of the model is illustrated completely.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12090" xmlns="http://purl.org/rss/1.0/"><title>Investigations on Material and Mechanical Properties, Air-Permeation Behavior and Filtration Performance of Mullite-Bonded Porous SiC Ceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12090</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Investigations on Material and Mechanical Properties, Air-Permeation Behavior and Filtration Performance of Mullite-Bonded Porous SiC Ceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Atanu Dey, Nijhuma Kayal, Omprakash Chakrabarti, Rafael Falchi Caldato, Murilo Daniel de Mello Innocentini, Vadila Giovana Guerra</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-28T10:19:49.686131-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12090</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12090</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12090</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A theoretical relation between processing parameters and porosity (29–56%) of mullite-bonded porous SiC ceramics was derived and validated with experimental data. Porosity-dependent variation of fracture strength (9–34 MPa) and elastic modulus (7–28 GPa) was explained by the minimum solid area model. At room temperature, the Darcian, <em>k</em><sub>1</sub> (1.2 × 10<sup>−13</sup>–1.6 × 10<sup>−12</sup> m<sup>2</sup>) and the non-Darcian, <em>k</em><sub>2</sub> (4.6 × 10<sup>−9</sup>–2.7 × 10<sup>−7</sup> m) permeability coefficients showed linear variation with porosity. Tests conducted up to 650°C indicated an increase in <em>k</em><sub>1</sub> with temperature and a reverse trend for <em>k</em><sub>2</sub>. Airborne NaCl nanoparticle filtration tests showed good performance of SiC ceramics with fractional collection efficiency of &gt;99% at 46–56% porosity levels.</p></div>
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A theoretical relation between processing parameters and porosity (29–56%) of mullite-bonded porous SiC ceramics was derived and validated with experimental data. Porosity-dependent variation of fracture strength (9–34 MPa) and elastic modulus (7–28 GPa) was explained by the minimum solid area model. At room temperature, the Darcian, k1 (1.2 × 10−13–1.6 × 10−12 m2) and the non-Darcian, k2 (4.6 × 10−9–2.7 × 10−7 m) permeability coefficients showed linear variation with porosity. Tests conducted up to 650°C indicated an increase in k1 with temperature and a reverse trend for k2. Airborne NaCl nanoparticle filtration tests showed good performance of SiC ceramics with fractional collection efficiency of &gt;99% at 46–56% porosity levels.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12126" xmlns="http://purl.org/rss/1.0/"><title>Effects of Postdensification Annealing on Microwave Dielectric Properties of Ba([Mg1−xCox]1/3Nb2/3)O3 Ceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12126</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effects of Postdensification Annealing on Microwave Dielectric Properties of Ba([Mg1−xCox]1/3Nb2/3)O3 Ceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Tu Lai Sun, Lei Li, Min Min Mao, Xiang Ming Chen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-28T10:19:34.305484-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12126</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12126</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12126</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Effects of postdensification annealing on microwave dielectric properties of Ba([Mg<sub>1−<em>x</em></sub>Co<sub><em>x</em></sub>]<sub>1/3</sub>Nb<sub>2/3</sub>)O<sub>3</sub> ceramics have been investigated. The 1:2 ordered complex perovskite structure is obtained in the entire composition range of the as-sintered samples, and the ordering degree decreases with increasing <em>x</em>. With increasing <em>x</em>, the dielectric constant (ε<sub>r</sub>) increases, the temperature coefficient of resonant frequency (τ<sub><em>f</em></sub>) shifts toward negative and can be tuned to near-zero for <em>x </em>=<em> </em>0.6, while the Q × <em>f</em> value decreases. With postdensification annealing at 1400°C in air for 24 h, the ordering degree increases, and Q × <em>f</em> value can be significantly improved without obvious change in ε<sub>r</sub>, while the composition for obtaining near-zero τ<sub><em>f</em></sub> shifts to <em>x </em>=<em> </em>0.8. Annealing at 1375°C and 1425°C in air for 24 h does not improve microwave dielectric properties more than annealing at 1400°C. A good combination of microwave dielectric properties of Ba([Mg<sub>1−<em>x</em></sub>Co<sub><em>x</em></sub>]<sub>1/3</sub>Nb<sub>2/3</sub>)O<sub>3</sub> ceramics after postdensification annealing at 1400°C in air for 24 h has been obtained for <em>x </em>=<em> </em>0.8: ε<sub>r</sub> = 31.7, Q × <em>f </em>=<em> </em>76,900 GHz, τ<sub><em>f</em></sub> = 3.3 ppm/°C.</p></div>
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Effects of postdensification annealing on microwave dielectric properties of Ba([Mg1−xCox]1/3Nb2/3)O3 ceramics have been investigated. The 1:2 ordered complex perovskite structure is obtained in the entire composition range of the as-sintered samples, and the ordering degree decreases with increasing x. With increasing x, the dielectric constant (εr) increases, the temperature coefficient of resonant frequency (τf) shifts toward negative and can be tuned to near-zero for x = 0.6, while the Q × f value decreases. With postdensification annealing at 1400°C in air for 24 h, the ordering degree increases, and Q × f value can be significantly improved without obvious change in εr, while the composition for obtaining near-zero τf shifts to x = 0.8. Annealing at 1375°C and 1425°C in air for 24 h does not improve microwave dielectric properties more than annealing at 1400°C. A good combination of microwave dielectric properties of Ba([Mg1−xCox]1/3Nb2/3)O3 ceramics after postdensification annealing at 1400°C in air for 24 h has been obtained for x = 0.8: εr = 31.7, Q × f = 76,900 GHz, τf = 3.3 ppm/°C.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12117" xmlns="http://purl.org/rss/1.0/"><title>Processing and Properties of BioCeramic Coatings onto 3D Ti-Mesh by DipCasting Method</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12117</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Processing and Properties of BioCeramic Coatings onto 3D Ti-Mesh by DipCasting Method</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Wei Yi, Xiaozhi Hu, Xudong Sun, Paul Ichim, Alexandra Suvorova</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-22T10:43:05.780098-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12117</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12117</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12117</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="ijac12117-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p>This study presents a dipcasting method that can deposit both porous and dense bioceramic coatings onto 3D Ti-mesh made from commercially pure Ti-mesh for surgical applications. First, a dense bioglass coating was deposited onto the 3D Ti-mesh, which is to seal off the Ti-mesh. Second, a microporous HA/bioglass coating was deposited on top of the dense bioglass coating, which is to promote bone regeneration into the 3D Ti-mesh. X-ray diffraction, field emission scanning electron microscopy, and energy dispersive X-ray spectroscopy were used to analyze the bioceramic coatings and cross-sectional microstructures. Vickers microhardness across the interface between bioceramic coating and Ti-substrate was measured.</p></div></div>
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This study presents a dipcasting method that can deposit both porous and dense bioceramic coatings onto 3D Ti-mesh made from commercially pure Ti-mesh for surgical applications. First, a dense bioglass coating was deposited onto the 3D Ti-mesh, which is to seal off the Ti-mesh. Second, a microporous HA/bioglass coating was deposited on top of the dense bioglass coating, which is to promote bone regeneration into the 3D Ti-mesh. X-ray diffraction, field emission scanning electron microscopy, and energy dispersive X-ray spectroscopy were used to analyze the bioceramic coatings and cross-sectional microstructures. Vickers microhardness across the interface between bioceramic coating and Ti-substrate was measured.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12114" xmlns="http://purl.org/rss/1.0/"><title>A Comparative Study of Densification of Sol-Gel-Derived Nano-Mullite due to the Influence of Iron, Nickel and Copper Ions</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12114</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A Comparative Study of Densification of Sol-Gel-Derived Nano-Mullite due to the Influence of Iron, Nickel and Copper Ions</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Debasis Roy, Biswajoy Bagchi, Alakananda Bhattacharya, Sukhen Das, Papiya Nandy</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-15T11:34:11.675282-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12114</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12114</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12114</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>By sol-gel process, mullite samples doped with 0.002<em>M</em>, 0.02<em>M</em>, 0.1<em>M</em>, 0.15<em>M</em>, and 0.2<em>M</em> of iron, nickel, and copper are prepared. Prepared gels were then dried, grinded, pressed into pellets, and sintered at temperatures 1000°C and 1300°C for 4 h. Mullite densification behavior was analyzed. Our intention is to study the role of metal ions in influencing mullitization behavior in the case of the sol-gel reaction process, to provide useful information of mullite. This study deals with the effect of metal ions on mullite formation, microstructure, and densification behavior in single-phase sol-gel-derived mullite.</p></div>
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By sol-gel process, mullite samples doped with 0.002M, 0.02M, 0.1M, 0.15M, and 0.2M of iron, nickel, and copper are prepared. Prepared gels were then dried, grinded, pressed into pellets, and sintered at temperatures 1000°C and 1300°C for 4 h. Mullite densification behavior was analyzed. Our intention is to study the role of metal ions in influencing mullitization behavior in the case of the sol-gel reaction process, to provide useful information of mullite. This study deals with the effect of metal ions on mullite formation, microstructure, and densification behavior in single-phase sol-gel-derived mullite.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12118" xmlns="http://purl.org/rss/1.0/"><title>Degradation and Mechanical Properties of Zirconia 3-Unit Fixed Dental Prostheses Machined on a CAD/CAM System</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12118</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Degradation and Mechanical Properties of Zirconia 3-Unit Fixed Dental Prostheses Machined on a CAD/CAM System</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Carlos Nelson Elias, Andréa Matos Melo, Heraldo Elias Salomão dos Santos, Claudinei dos Santos</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-15T11:33:53.738824-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12118</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12118</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12118</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="ijac12118-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p>The manufacturing of ceramics fixed dental prostheses (FDPs) is not the same as that of standardized samples and, therefore, the surface finishing are not necessarily the same in both cases. Standardized samples and FDPs were sintered, polished, hydrothermally aged in saliva, and submitted to mechanical tests. The results showed a difference in bending strength between machined (911.19 MPa) and polished FDPs (573.84 MPa). ANOVA statistical analysis did not show a difference in flexural strength between nondegraded (911.19 MPa) and degraded (871.94 MPa) FDPs. No differences were found in the bending strength and toughness of standardized samples and FDPs.</p></div></div>
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The manufacturing of ceramics fixed dental prostheses (FDPs) is not the same as that of standardized samples and, therefore, the surface finishing are not necessarily the same in both cases. Standardized samples and FDPs were sintered, polished, hydrothermally aged in saliva, and submitted to mechanical tests. The results showed a difference in bending strength between machined (911.19 MPa) and polished FDPs (573.84 MPa). ANOVA statistical analysis did not show a difference in flexural strength between nondegraded (911.19 MPa) and degraded (871.94 MPa) FDPs. No differences were found in the bending strength and toughness of standardized samples and FDPs.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12115" xmlns="http://purl.org/rss/1.0/"><title>3rd Ceramic Leadership Summit</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12115</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">3rd Ceramic Leadership Summit</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Marina R. Pascucci</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-14T10:16:49.713744-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12115</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12115</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12115</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The Ceramic Leadership Summit is designed to explore business opportunities, emerging technologies, and critical issues that challenge the ceramic and glass materials community. In 2012, the 3rd Ceramic Leadership Summit was held in conjunction with the 4th International Congress on Ceramics (ICC4). The one-day program focused on technology transfer, entrepreneurship, and product innovation. Important topics discussed included strategies for creating and sustaining a small business, intellectual property protection, technology transfer, and mechanisms for government–university–industry partnerships. International speakers in the case study session addressed these topics from the perspective of their local and national policies and practices. Several of the case study presentations highlighted the use of “waste materials” in the creation and application of new technologies and products.</p></div>
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The Ceramic Leadership Summit is designed to explore business opportunities, emerging technologies, and critical issues that challenge the ceramic and glass materials community. In 2012, the 3rd Ceramic Leadership Summit was held in conjunction with the 4th International Congress on Ceramics (ICC4). The one-day program focused on technology transfer, entrepreneurship, and product innovation. Important topics discussed included strategies for creating and sustaining a small business, intellectual property protection, technology transfer, and mechanisms for government–university–industry partnerships. International speakers in the case study session addressed these topics from the perspective of their local and national policies and practices. Several of the case study presentations highlighted the use of “waste materials” in the creation and application of new technologies and products.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12119" xmlns="http://purl.org/rss/1.0/"><title>Low-Temperature Sintering Microwave Characteristics of B2O3-doped CaLa4Ti4O15 Dielectric Ceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12119</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Low-Temperature Sintering Microwave Characteristics of B2O3-doped CaLa4Ti4O15 Dielectric Ceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Cheng-Hsing Hsu, Ci-Jie Huang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-13T10:47:24.913214-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12119</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12119</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12119</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Preparation and microwave dielectric properties of B<sub>2</sub>O<sub>3</sub>-doped CaLa<sub>4</sub>Ti<sub>4</sub>O<sub>15</sub> ceramics have been investigated. X-ray diffraction data show that CaLa<sub>4</sub>Ti<sub>4</sub>O<sub>15</sub> ceramic has a trigonal structure coupled with a second phase of CaLa<sub>4</sub>Ti<sub>5</sub>O<sub>17</sub>. The CaLa<sub>4</sub>Ti<sub>4</sub>O<sub>15</sub> ceramic with addition of 0.5 wt% B<sub>2</sub>O<sub>3</sub>, sintered at 1220°C for 4 h, exhibits microwave dielectric properties with a dielectric constant of 45.8, <em>Q × f</em> value of 24,000 GHz, and temperature coefficient of resonant frequency (τ<sub><em>f</em></sub>) of −19 ppm/<sup>°</sup>C. B<sub>2</sub>O<sub>3</sub>-doped CaLa<sub>4</sub>Ti<sub>4</sub>O<sub>15</sub> ceramics, which have better sintering behavior (decrease in sintering temperature ~ 330°C) and dielectric properties than pure CaLa<sub>4</sub>Ti<sub>4</sub>O<sub>15</sub> ceramics, are candidates for applications in microwave devices.</p></div>
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Preparation and microwave dielectric properties of B2O3-doped CaLa4Ti4O15 ceramics have been investigated. X-ray diffraction data show that CaLa4Ti4O15 ceramic has a trigonal structure coupled with a second phase of CaLa4Ti5O17. The CaLa4Ti4O15 ceramic with addition of 0.5 wt% B2O3, sintered at 1220°C for 4 h, exhibits microwave dielectric properties with a dielectric constant of 45.8, Q × f value of 24,000 GHz, and temperature coefficient of resonant frequency (τf) of −19 ppm/°C. B2O3-doped CaLa4Ti4O15 ceramics, which have better sintering behavior (decrease in sintering temperature ~ 330°C) and dielectric properties than pure CaLa4Ti4O15 ceramics, are candidates for applications in microwave devices.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12113" xmlns="http://purl.org/rss/1.0/"><title>Slurry-based Additive Manufacturing of Ceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12113</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Slurry-based Additive Manufacturing of Ceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Thomas Mühler, Cynthia M. Gomes, Jürgen Heinrich, Jens Günster</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-13T10:47:16.776313-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12113</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12113</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12113</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Most additive manufacturing (AM) techniques have in common that material is spread out as thin layers of a dried powder/granulate by a roller or a shaker system. These layers are mostly characterized by a low packing rate. On the other hand, appreciable densities can be reached by the use of ceramic slurries. In this context, the layer-wise slurry deposition (LSD) has been developed. Specific features of the LSD process are reflected on the basis of already existing additive manufacturing technologies. The microstructure of laser-sintered bodies will be discussed, and strategies for an improved microstructure during sintering will be introduced.</p></div>
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Most additive manufacturing (AM) techniques have in common that material is spread out as thin layers of a dried powder/granulate by a roller or a shaker system. These layers are mostly characterized by a low packing rate. On the other hand, appreciable densities can be reached by the use of ceramic slurries. In this context, the layer-wise slurry deposition (LSD) has been developed. Specific features of the LSD process are reflected on the basis of already existing additive manufacturing technologies. The microstructure of laser-sintered bodies will be discussed, and strategies for an improved microstructure during sintering will be introduced.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12111" xmlns="http://purl.org/rss/1.0/"><title>Microstructure Modifications and Sintering Mechanism of Ba0.55Sr0.4Ca0.05TiO3 Ceramics Containing Different MgO Additive for LTCC Application</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12111</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Microstructure Modifications and Sintering Mechanism of Ba0.55Sr0.4Ca0.05TiO3 Ceramics Containing Different MgO Additive for LTCC Application</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dahao Wang, Xiaolei Li, Qianqian Jia, Yugui Zhou, Huiming Ji, Yejing Dai</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-13T10:47:11.850727-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12111</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12111</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12111</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Ferroelectric Ba<sub>0.55</sub>Sr<sub>0.4</sub>Ca<sub>0.05</sub>TiO<sub>3</sub> (BSCT) ceramics with nano-MgO additive have been prepared by typical electrical ceramic technology sintered at 950°C for 2 h. The influence of the additive content on the sintering behaviors of BSCT ceramics is investigated. The results show that the interactions of MgO with BSCT and B<sub>2</sub>O<sub>3</sub>-Li<sub>2</sub>O liquid sintering additive help to form wetting boundaries for accelerating densification process, promote the grain growth of BSCT ceramic. The BSCT ceramic with 20 wt% nano-MgO possesses uniform microstructure, high densification, and superior dielectric properties. The modification mechanism of nano-MgO on BSCT ceramic is summarized as “MgO assisted wetting sintering model.”</p></div>
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Ferroelectric Ba0.55Sr0.4Ca0.05TiO3 (BSCT) ceramics with nano-MgO additive have been prepared by typical electrical ceramic technology sintered at 950°C for 2 h. The influence of the additive content on the sintering behaviors of BSCT ceramics is investigated. The results show that the interactions of MgO with BSCT and B2O3-Li2O liquid sintering additive help to form wetting boundaries for accelerating densification process, promote the grain growth of BSCT ceramic. The BSCT ceramic with 20 wt% nano-MgO possesses uniform microstructure, high densification, and superior dielectric properties. The modification mechanism of nano-MgO on BSCT ceramic is summarized as “MgO assisted wetting sintering model.”
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12116" xmlns="http://purl.org/rss/1.0/"><title>Effects of ZnO–B2O3 Addition on the Microstructure and Microwave Properties of Low-Temperature Sintered Barium Strontium Titanate (BST) Thick Films</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12116</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effects of ZnO–B2O3 Addition on the Microstructure and Microwave Properties of Low-Temperature Sintered Barium Strontium Titanate (BST) Thick Films</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Christian Kohler, Andreas Friederich, Mohsen Sazegar, Mohammad Nikfalazar, Florian Stemme, Di Wang, Christian Kuebel, Rolf Jakoby, Joachim R. Binder</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-13T10:47:10.924381-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12116</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12116</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12116</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>BST–ZnO–B<sub>2</sub>O<sub>3</sub>–composite thick films have been investigated regarding their suitability as low-temperature sintered tunable microwave dielectrics. The investigations showed that already a small amount of ZnO–B<sub>2</sub>O<sub>3</sub> additive can remarkably reduce the sintering temperature down to 900°C. Microstructural investigations of the thick films revealed the formation of an amorphous intergranular phase and a clustering of particles for high additive amounts. The microwave characterization showed a reduction in relative permittivity, dielectric loss, and tunability of the thick films with increasing additive content. These results demonstrate the potential to tailor the material abilities by varying the additive content.</p></div>
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BST–ZnO–B2O3–composite thick films have been investigated regarding their suitability as low-temperature sintered tunable microwave dielectrics. The investigations showed that already a small amount of ZnO–B2O3 additive can remarkably reduce the sintering temperature down to 900°C. Microstructural investigations of the thick films revealed the formation of an amorphous intergranular phase and a clustering of particles for high additive amounts. The microwave characterization showed a reduction in relative permittivity, dielectric loss, and tunability of the thick films with increasing additive content. These results demonstrate the potential to tailor the material abilities by varying the additive content.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12110" xmlns="http://purl.org/rss/1.0/"><title>Synthesis of CoFe2O4 Nanoparticles by a Low Temperature Microwave-Assisted Ball-Milling Technique</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12110</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Synthesis of CoFe2O4 Nanoparticles by a Low Temperature Microwave-Assisted Ball-Milling Technique</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ding Chen, Xiang Yi, Zhenhua Chen, Yingzhe Zhang, Biyu Chen, Zhitao Kang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-10T10:40:34.363102-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12110</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12110</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12110</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Well-crystallized Cobalt ferrite nanoparticles with mean size of 20 nm and high saturation magnetization (82.9 emu/g) were synthesized at a low temperature (≤100°C) by microwave-assisted solid–liquid reaction ball-milling technique without subsequent calcination. CoC<sub>2</sub>O<sub>4</sub>·4H<sub>2</sub>O and Fe powder were used as raw materials and stainless steel or pure iron milling balls with diameter of 1.5 mm were used. As a contrast, solid–liquid reaction ball milling without microwave assistance was also investigated. The results showed that this is a simple, environmentally friendly, and energy-saving technique for ferrite nanocrystal synthesis.</p></div>
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Well-crystallized Cobalt ferrite nanoparticles with mean size of 20 nm and high saturation magnetization (82.9 emu/g) were synthesized at a low temperature (≤100°C) by microwave-assisted solid–liquid reaction ball-milling technique without subsequent calcination. CoC2O4·4H2O and Fe powder were used as raw materials and stainless steel or pure iron milling balls with diameter of 1.5 mm were used. As a contrast, solid–liquid reaction ball milling without microwave assistance was also investigated. The results showed that this is a simple, environmentally friendly, and energy-saving technique for ferrite nanocrystal synthesis.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12112" xmlns="http://purl.org/rss/1.0/"><title>Homogeneous Precipitation Synthesis and Low-Voltage Cathodoluminescence of SnO2:Eu3+ Phosphors for Field Emission Displays</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12112</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Homogeneous Precipitation Synthesis and Low-Voltage Cathodoluminescence of SnO2:Eu3+ Phosphors for Field Emission Displays</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Tongwen Huang, Xiaojun Wang, Pingping Zhu, Huili Li, Tao Feng, Zhuo Sun</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-10T10:40:26.189289-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12112</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12112</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12112</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A reddish-orange-emitting <span class="fixed-roman">SnO<sub>2</sub>:Eu<sup>3+</sup></span> phosphor for field emission displays (FEDs) was successfully synthesized via a homogeneous precipitation route using urea as a precipitant. The influences of the dopant concentration of <span class="fixed-roman">Eu<sup>3+</sup></span> and calcination temperature on optical properties were investigated. The low-voltage field emission properties of the FED device prepared using the synthesized <span class="fixed-roman">SnO<sub>2</sub>:Eu<sup>3+</sup></span> phosphors were reported. Under the UV light, <span class="fixed-roman">SnO<sub>2</sub>:Eu<sup>3+</sup></span> phosphors display the strong orange–red emission peaked at 587, 591, and 597 nm due to the <sup>5</sup>D<sub>0</sub>→<sup>7</sup>F<sub>1</sub> magnetic dipole transition of <span class="fixed-roman">Eu<sup>3+</sup></span>. The phosphor doped with 1.0 mol% <span class="fixed-roman">Eu<sup>3+</sup></span> possesses the highest photoluminescent (PL) intensity. Under the low-voltage excitation of 300 V, the fabricated FED device exhibits the bright orange–red emission, high-voltage brightness saturation, and high color purity, which has a potential application in low-voltage full color FEDs.</p></div>
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A reddish-orange-emitting SnO2:Eu3+ phosphor for field emission displays (FEDs) was successfully synthesized via a homogeneous precipitation route using urea as a precipitant. The influences of the dopant concentration of Eu3+ and calcination temperature on optical properties were investigated. The low-voltage field emission properties of the FED device prepared using the synthesized SnO2:Eu3+ phosphors were reported. Under the UV light, SnO2:Eu3+ phosphors display the strong orange–red emission peaked at 587, 591, and 597 nm due to the 5D0→7F1 magnetic dipole transition of Eu3+. The phosphor doped with 1.0 mol% Eu3+ possesses the highest photoluminescent (PL) intensity. Under the low-voltage excitation of 300 V, the fabricated FED device exhibits the bright orange–red emission, high-voltage brightness saturation, and high color purity, which has a potential application in low-voltage full color FEDs.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12109" xmlns="http://purl.org/rss/1.0/"><title>Fracture Resistance Behavior of High-Thermal-Conductivity Silicon Nitride Ceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12109</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Fracture Resistance Behavior of High-Thermal-Conductivity Silicon Nitride Ceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">You Zhou, Tatsuki Ohji, Hideki Hyuga, Yu-ichi Yoshizawa, Norimitsu Murayama, Kiyoshi Hirao</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-03T10:51:45.766953-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12109</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12109</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12109</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Silicon nitride ceramics were prepared from a high-purity silicon powder doped with 2 mol% Y<sub>2</sub>O<sub>3</sub> and 5 mol% MgO as sintering additives via a route of sintering of reaction-bonded silicon nitride (SRBSN). The materials sintered at 1900°C for 3, 6, 12, and 24 h had thermal conductivities of 109, 125, 146, and 154 W/m/K, and four-point bending strengths of 786, 676, 608, and 505 MPa, respectively. The fracture toughness values, determined by the single-edge-precracked-beam (SEPB) method, were 8.4, 8.6, 9.7, and 10.7 MPa m<sup>1/2</sup> for the materials sintered for 3, 6, 12, and 24 h, respectively, which were similar to the results measured by the chevron-notched-beam (CNB) test method. The materials sintered for longer times (12 and 24 h) showed stronger <em>R</em>-curve behaviors over longer range of crack extension, in comparison with the materials sintered for shorter times (3 and 6 h).</p></div>
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Silicon nitride ceramics were prepared from a high-purity silicon powder doped with 2 mol% Y2O3 and 5 mol% MgO as sintering additives via a route of sintering of reaction-bonded silicon nitride (SRBSN). The materials sintered at 1900°C for 3, 6, 12, and 24 h had thermal conductivities of 109, 125, 146, and 154 W/m/K, and four-point bending strengths of 786, 676, 608, and 505 MPa, respectively. The fracture toughness values, determined by the single-edge-precracked-beam (SEPB) method, were 8.4, 8.6, 9.7, and 10.7 MPa m1/2 for the materials sintered for 3, 6, 12, and 24 h, respectively, which were similar to the results measured by the chevron-notched-beam (CNB) test method. The materials sintered for longer times (12 and 24 h) showed stronger R-curve behaviors over longer range of crack extension, in comparison with the materials sintered for shorter times (3 and 6 h).
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12088" xmlns="http://purl.org/rss/1.0/"><title>Effect of Water Content of Synthetic Hydrogel on Dehydration Performance of Nanoporous LTA Zeolite Membranes</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12088</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of Water Content of Synthetic Hydrogel on Dehydration Performance of Nanoporous LTA Zeolite Membranes</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Saeed Shirazian, Soheila Ghafarnejad Parto, Seyed Nezameddin Ashrafizadeh</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-03T10:51:34.244236-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12088</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12088</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12088</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Nanoporous LTA-type zeolite membranes were synthesized on α-Al<sub>2</sub>O<sub>3</sub> disk as substrate using secondary growth method. A gel formula of 1 Al<sub>2</sub>O<sub>3</sub>: 2 SiO<sub>2</sub>: 3.4 Na<sub>2</sub>O: W H<sub>2</sub>O in molar basis was chosen while its water content (W) was varied. Four levels of water contents of 140, 155, 175, and 200 were selected for membrane synthesis. The results showed that the best membrane was synthesized with water content of 155. The most efficient zeolite membrane showed a permeation flux of 0.5 kg/m<sup>2</sup>/h and a separation factor of 3800 in dehydration of a 5/95 (wt%) water/isopropanol mixture at 298 K.</p></div>
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Nanoporous LTA-type zeolite membranes were synthesized on α-Al2O3 disk as substrate using secondary growth method. A gel formula of 1 Al2O3: 2 SiO2: 3.4 Na2O: W H2O in molar basis was chosen while its water content (W) was varied. Four levels of water contents of 140, 155, 175, and 200 were selected for membrane synthesis. The results showed that the best membrane was synthesized with water content of 155. The most efficient zeolite membrane showed a permeation flux of 0.5 kg/m2/h and a separation factor of 3800 in dehydration of a 5/95 (wt%) water/isopropanol mixture at 298 K.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12075" xmlns="http://purl.org/rss/1.0/"><title>Surface Modification of Alumina/ Zirconia Ceramics Upon Different Fluoride-Based Treatments</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12075</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Surface Modification of Alumina/ Zirconia Ceramics Upon Different Fluoride-Based Treatments</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Simona Cavalu, Florin Banica, Viorica Simon, Ipek Akin, Gultekin Goller</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-02T13:12:21.963655-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12075</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12075</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12075</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The aim of this study was to prepare and to characterize the structure of Al<sub>2</sub>O<sub>3</sub>–3YSZ composites with 5% TiO<sub>2</sub> addition as well as the surface modification upon treatments with SnF<sub>2</sub> and NaBF<sub>4</sub>, respectively. SEM micrographs showed the controlled densification of the composites as an effect of 3YSZ and TiO<sub>2</sub> addition to alumina matrix. By FTIR and XRD, the characteristics of Al-O and Zr-O vibrations, respectively, the diffractions lines related to α-corundum and zirconia in tetragonal phase were discussed. Qualitative and quantitative results obtained by XPS and ATR FTIR demonstrated that the proposed materials are more sensitive to SnF<sub>2</sub> than to NaBF<sub>4</sub> treatment.</p></div>
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The aim of this study was to prepare and to characterize the structure of Al2O3–3YSZ composites with 5% TiO2 addition as well as the surface modification upon treatments with SnF2 and NaBF4, respectively. SEM micrographs showed the controlled densification of the composites as an effect of 3YSZ and TiO2 addition to alumina matrix. By FTIR and XRD, the characteristics of Al-O and Zr-O vibrations, respectively, the diffractions lines related to α-corundum and zirconia in tetragonal phase were discussed. Qualitative and quantitative results obtained by XPS and ATR FTIR demonstrated that the proposed materials are more sensitive to SnF2 than to NaBF4 treatment.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12093" xmlns="http://purl.org/rss/1.0/"><title>Characterization of Magnesium-Doped Hydroxyapatite Prepared by Sol-Gel Process</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12093</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Characterization of Magnesium-Doped Hydroxyapatite Prepared by Sol-Gel Process</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Salima Ziani, Samira Meski, Hafit Khireddine</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-30T10:24:19.451459-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12093</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12093</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12093</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Pure and doped hydroxyapatite (HA) nanocrystalline powders (Ca<sub>10-x</sub>Mg<sub>x</sub>(PO<sub>4</sub>)<sub>6</sub>OH<sub>2</sub>) were synthesized using sol-gel process. For this, calcium nitrate tetrahydrate, magnesium nitrate hexahydrate, and phosphorous pentoxide were used as precursors for Ca, Mg, and P, respectively. Calculated amounts of magnesium ions (Mg<sup>+2</sup>) especially from 0 to 10% (molar ratio) were incorporated as dopant into the calcium sol solution. The structure and morphology of the gels obtained after mixing the phosphorous and (calcium + magnesium) sol solution were different, and their condensations in time depend on the quantities of magnesium added. The several powders resulting from the gels dried and sintered at 500°C for 1 h were characterized by thermogravimetry (TG), Fourier transform infrared spectroscopy (FTIR), X-ray diffraction (XRD), and inductively coupled plasma (ICP). Additionally, their agglomeration, morphology, and particle size were investigated using scanning electron microscopy (SEM) and transmission electron microscopy (TEM). The specific surface area of each sample was measured by the Brunauer–Emmett–Teller (BET) gas adsorption technique. The results of XRD, FTIR, and ICP values ranged between 0.45 and 2.11 mg/L indicated that the magnesium added in the calcium solution was incorporated in the lattice structure of HA so prepared, while those obtained by SEM and TEM confirmed the influence of Mg on their morphology (needle and irregular shape) and crystallite size, which is about 30–60 nm. The as-prepared powders had a specific surface area ranged between 6.37 and 27.60 m<sup>2</sup>/g.</p></div>
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Pure and doped hydroxyapatite (HA) nanocrystalline powders (Ca10-xMgx(PO4)6OH2) were synthesized using sol-gel process. For this, calcium nitrate tetrahydrate, magnesium nitrate hexahydrate, and phosphorous pentoxide were used as precursors for Ca, Mg, and P, respectively. Calculated amounts of magnesium ions (Mg+2) especially from 0 to 10% (molar ratio) were incorporated as dopant into the calcium sol solution. The structure and morphology of the gels obtained after mixing the phosphorous and (calcium + magnesium) sol solution were different, and their condensations in time depend on the quantities of magnesium added. The several powders resulting from the gels dried and sintered at 500°C for 1 h were characterized by thermogravimetry (TG), Fourier transform infrared spectroscopy (FTIR), X-ray diffraction (XRD), and inductively coupled plasma (ICP). Additionally, their agglomeration, morphology, and particle size were investigated using scanning electron microscopy (SEM) and transmission electron microscopy (TEM). The specific surface area of each sample was measured by the Brunauer–Emmett–Teller (BET) gas adsorption technique. The results of XRD, FTIR, and ICP values ranged between 0.45 and 2.11 mg/L indicated that the magnesium added in the calcium solution was incorporated in the lattice structure of HA so prepared, while those obtained by SEM and TEM confirmed the influence of Mg on their morphology (needle and irregular shape) and crystallite size, which is about 30–60 nm. The as-prepared powders had a specific surface area ranged between 6.37 and 27.60 m2/g.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12044" xmlns="http://purl.org/rss/1.0/"><title>Effect of Synthesis Route on Electrical and Electrochemical Performance of Nd1.8Ce0.2CuO4+δ Cathode Material for Intermediate-Temperature Solid Oxide Fuel Cells</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12044</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of Synthesis Route on Electrical and Electrochemical Performance of Nd1.8Ce0.2CuO4+δ Cathode Material for Intermediate-Temperature Solid Oxide Fuel Cells</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Anushree P. Khandale, Shyamsunder S. Bhoga</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-30T10:24:02.429774-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12044</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12044</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12044</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Nano-crystalline Nd<sub>1.8</sub>Ce<sub>0.2</sub>CuO<sub>4+δ</sub> synthesized by combusting mixed precursor materials under microwave heating followed by sintering at 1000°C for 4 h exhibits highest dc conductivity (σ = 2.50 S/cm at 700°C) due to lowest crystallite size (50 nm), which compared with preparation by conventional combustion and solid-state reaction. Symmetric cells configured as electrode/electrolyte/electrode were fabricated by spin coating. The lowest area specific resistance (ASR) value of 0.50 Ω cm<sup>2</sup> was obtained at a temperature 700°C. Morphology of cathode material is largely dependent on the preparative route, and that influences ASR. Low frequency complex impedance curve was modeled by Gerischer element. The electrochemical performance suggested absorption of oxygen by the Nd<sub>1.8</sub>Ce<sub>0.2</sub>CuO<sub>4+δ</sub> lattice. Combustion of precursors using microwave heating promises to be a potential route for materials preparation to achieve improved electrochemical performance of cathode in intermediate temperature solid oxide fuel cell applications.</p></div>
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Nano-crystalline Nd1.8Ce0.2CuO4+δ synthesized by combusting mixed precursor materials under microwave heating followed by sintering at 1000°C for 4 h exhibits highest dc conductivity (σ = 2.50 S/cm at 700°C) due to lowest crystallite size (50 nm), which compared with preparation by conventional combustion and solid-state reaction. Symmetric cells configured as electrode/electrolyte/electrode were fabricated by spin coating. The lowest area specific resistance (ASR) value of 0.50 Ω cm2 was obtained at a temperature 700°C. Morphology of cathode material is largely dependent on the preparative route, and that influences ASR. Low frequency complex impedance curve was modeled by Gerischer element. The electrochemical performance suggested absorption of oxygen by the Nd1.8Ce0.2CuO4+δ lattice. Combustion of precursors using microwave heating promises to be a potential route for materials preparation to achieve improved electrochemical performance of cathode in intermediate temperature solid oxide fuel cell applications.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12076" xmlns="http://purl.org/rss/1.0/"><title>Biological Performance of Calcium Pyrophosphate-coated Porous Alumina Scaffolds</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12076</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Biological Performance of Calcium Pyrophosphate-coated Porous Alumina Scaffolds</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Salma M. Naga, Mohamed Awaad, Hesham F. El-Maghraby, Abeer M. El-Kady</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-30T10:23:46.934193-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12076</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12076</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12076</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The present work aims at synthesis and study the bioactivity of porous alumina scaffolds coated with calcium pyrophosphate. Characterization of the formed calcium pyrophosphate and the coated scaffolds was assessed by X-ray diffraction analysis and scanning electron microscope examinations. The <em>in vivo</em> studies revealed the ability of the porous scaffolds to regenerate bone tissue in femur defects of albino rats. Histological analysis showed that the defect is almost entirely filled with new bone. The formed bone is characterized as a mature bone. The produced bone grafts are intended to be used as bone substitute or bone filler.</p></div>
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The present work aims at synthesis and study the bioactivity of porous alumina scaffolds coated with calcium pyrophosphate. Characterization of the formed calcium pyrophosphate and the coated scaffolds was assessed by X-ray diffraction analysis and scanning electron microscope examinations. The in vivo studies revealed the ability of the porous scaffolds to regenerate bone tissue in femur defects of albino rats. Histological analysis showed that the defect is almost entirely filled with new bone. The formed bone is characterized as a mature bone. The produced bone grafts are intended to be used as bone substitute or bone filler.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12066" xmlns="http://purl.org/rss/1.0/"><title>A Novel and Simple Process for Nanosized Mg-Mn Ferrite Preparation from Solution Combustion Method and Study of its Characteristics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12066</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A Novel and Simple Process for Nanosized Mg-Mn Ferrite Preparation from Solution Combustion Method and Study of its Characteristics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Nilar Lwin, Ahmad Fauzi Mohd Noor, Srimala Sreekantan, Radzali Othman, Aye Aye Thant</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-30T10:23:33.093229-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12066</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12066</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12066</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A novel solution combustion method has been used to prepare Mg-Mn ferrites of various compositions, Mg<sub>0.9</sub>Mn<sub>0.1</sub>Fe<sub>1-x</sub>O<sub>4</sub> where <em>x </em>=<em> </em>0.2, 0.4, 0.6, 0.8, and the properties were investigated in the present work. Nano-size Mg-Mn ferrite particles with diameter in the range of 8~ 15 nm were successfully formed via this method. The combustion temperature of the oxidation-reduction was apparently occurred at 200°C. The result of X-ray diffraction (XRD) analysis indicated that the as-burnt powder affords a pure single spinel ferrite phase at low temperature. The thermal analysis of nitrate–citrate gels was characterized by DTA-TG. The TEM and SEM observations give the morphology and microstructure of the products. The dielectric properties of the sintered Mg-Mn ferrites were investigated by using HP/Agilent 4291B RF impedence/material analyzer. It was found that there was no maximum dielectric loss within the measured frequency range until 1 GHz due to excellent compositional control in this method.</p></div>
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A novel solution combustion method has been used to prepare Mg-Mn ferrites of various compositions, Mg0.9Mn0.1Fe1-xO4 where x = 0.2, 0.4, 0.6, 0.8, and the properties were investigated in the present work. Nano-size Mg-Mn ferrite particles with diameter in the range of 8~ 15 nm were successfully formed via this method. The combustion temperature of the oxidation-reduction was apparently occurred at 200°C. The result of X-ray diffraction (XRD) analysis indicated that the as-burnt powder affords a pure single spinel ferrite phase at low temperature. The thermal analysis of nitrate–citrate gels was characterized by DTA-TG. The TEM and SEM observations give the morphology and microstructure of the products. The dielectric properties of the sintered Mg-Mn ferrites were investigated by using HP/Agilent 4291B RF impedence/material analyzer. It was found that there was no maximum dielectric loss within the measured frequency range until 1 GHz due to excellent compositional control in this method.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12085" xmlns="http://purl.org/rss/1.0/"><title>Reaction-Bonded Boron Carbide/Magnesium–Silicon Composites</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12085</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Reaction-Bonded Boron Carbide/Magnesium–Silicon Composites</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Matan Cafri, Alon Malka, Helen Dilman, Moshe P. Dariel, Nahum Frage</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-30T10:23:14.962212-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12085</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12085</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12085</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Reaction-bonded boron carbide was manufactured by infiltrating porous boron carbide preforms at 1273 K with a Mg-Si eutectic alloy. The resulting composite material consists, in addition to the original B<sub>4</sub>C, of SiC, Mg<sub>2</sub>Si, and a Mg-rich complex boride/carbide Mg<sub>x</sub>(Al,Si)<sub>y</sub>(B,C)<sub>z</sub> phase. The composites display high hardness (1700 HV), Young's modulus (356 MPa) and a moderate bending strength (230 MPa). The ballistic efficiency (of about 6.7), as determined by the depth of penetration method, is much higher than that of alumina and similar to that of silicon-infiltrated reaction-bonded composites.</p></div>
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Reaction-bonded boron carbide was manufactured by infiltrating porous boron carbide preforms at 1273 K with a Mg-Si eutectic alloy. The resulting composite material consists, in addition to the original B4C, of SiC, Mg2Si, and a Mg-rich complex boride/carbide Mgx(Al,Si)y(B,C)z phase. The composites display high hardness (1700 HV), Young's modulus (356 MPa) and a moderate bending strength (230 MPa). The ballistic efficiency (of about 6.7), as determined by the depth of penetration method, is much higher than that of alumina and similar to that of silicon-infiltrated reaction-bonded composites.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12072" xmlns="http://purl.org/rss/1.0/"><title>Phase Evolution of Solid-State BaTiO3 Powder Prepared by Different Starting BaCO3</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12072</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Phase Evolution of Solid-State BaTiO3 Powder Prepared by Different Starting BaCO3</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ting-Tai Lee, Chi-Yuen Huang, Che-Yuan Chang, I-Kuan Cheng, Ching-Li Hu, Che-Yi Su, Chun-Te Lee, Masayuki Fujimoto</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-30T10:21:10.462661-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12072</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12072</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12072</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Two different specific surface area of starting BaCO<sub>3,</sub> 10 and 30 m<sup>2</sup>/g, are used to prepare solid-state BaTiO<sub>3</sub> powder. Pure tetragonal BaTiO<sub>3</sub> was obtained at a lower calcination temperature with smaller BaCO<sub>3</sub>, and the kinetic calculations of activation energy also agree with it. A clear, thin, and nano-sized cubic BaTiO<sub>3</sub> clusters on TiO<sub>2</sub> particles were also observed. A narrower particle size distribution of BaTiO<sub>3</sub> powder (350 nm) was obtained from 30 m<sup>2</sup>/g of starting BaCO<sub>3</sub> at 1000°C. After sintering with reducing atmosphere, the ceramics with potential of X8R or X7R specifications and a clear core–shell microstructure were obtained in this study.</p></div>
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Two different specific surface area of starting BaCO3, 10 and 30 m2/g, are used to prepare solid-state BaTiO3 powder. Pure tetragonal BaTiO3 was obtained at a lower calcination temperature with smaller BaCO3, and the kinetic calculations of activation energy also agree with it. A clear, thin, and nano-sized cubic BaTiO3 clusters on TiO2 particles were also observed. A narrower particle size distribution of BaTiO3 powder (350 nm) was obtained from 30 m2/g of starting BaCO3 at 1000°C. After sintering with reducing atmosphere, the ceramics with potential of X8R or X7R specifications and a clear core–shell microstructure were obtained in this study.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12094" xmlns="http://purl.org/rss/1.0/"><title>A Novel Si3N4–SiC Ceramic Used for Volumetric Receivers</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12094</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A Novel Si3N4–SiC Ceramic Used for Volumetric Receivers</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jianfeng Wu, Meng Liu, Xiaohong Xu, Yaxiang Zhang, Xinbin Lao</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-29T10:10:35.105002-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12094</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12094</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12094</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Si<sub>3</sub>N<sub>4</sub>–SiC composite ceramics used for volumetric receivers were fabricated by pressureless sintering of micrometer SiC, Si<sub>3</sub>N<sub>4</sub>, andalusite, and other minor additions powders. Mechanical, thermal expansion, thermal conductivity, and thermal shock resistance properties were tested at different sintering temperatures. The best sintering temperature of optimum formula A2 is 1360°C, and the bending strength reaches 79.60 Mpa. And moreover, its thermal expansion coefficient is 6.401 × 10<sup>−6</sup>/°C, thermal conductivity is 7.83 W/(m K), and no crack occurs even subjected to 30 cycles thermal shock with a bending strength increase rate of 4.72%. X-ray diffraction results show that the phase constituents of the sintered products mainly consist of SiC, Si<sub>3</sub>N<sub>4</sub>, mullite, and quartz. Microstructure that is most appropriate and exhibits maximal thermal shock resistance was detected using SEM. The porosity of Si<sub>3</sub>N<sub>4</sub>–SiC ceramic foam prepared from formula A2 is 95%, which provides a rapid and steady action for the receiver. The evaluation of the present foam shows that Si<sub>3</sub>N<sub>4</sub>–SiC ceramic composite is a good candidate for volumetric receivers.</p></div>
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Si3N4–SiC composite ceramics used for volumetric receivers were fabricated by pressureless sintering of micrometer SiC, Si3N4, andalusite, and other minor additions powders. Mechanical, thermal expansion, thermal conductivity, and thermal shock resistance properties were tested at different sintering temperatures. The best sintering temperature of optimum formula A2 is 1360°C, and the bending strength reaches 79.60 Mpa. And moreover, its thermal expansion coefficient is 6.401 × 10−6/°C, thermal conductivity is 7.83 W/(m K), and no crack occurs even subjected to 30 cycles thermal shock with a bending strength increase rate of 4.72%. X-ray diffraction results show that the phase constituents of the sintered products mainly consist of SiC, Si3N4, mullite, and quartz. Microstructure that is most appropriate and exhibits maximal thermal shock resistance was detected using SEM. The porosity of Si3N4–SiC ceramic foam prepared from formula A2 is 95%, which provides a rapid and steady action for the receiver. The evaluation of the present foam shows that Si3N4–SiC ceramic composite is a good candidate for volumetric receivers.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12101" xmlns="http://purl.org/rss/1.0/"><title>Failure Analysis of Modern Silicon Dice</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12101</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Failure Analysis of Modern Silicon Dice</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Roberto Dugnani, Paul Verghese</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-29T10:10:25.319727-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12101</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12101</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12101</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Although the utilization of silicon dice in electronic devices has been in place for approximately 50 years, its widespread application has occurred more recently with the rapid expansion of the consumer markets for digital devices such as cameras, personal computers, video players, and smart phones. In particular, due to the recent market drive in the miniaturization and cost reduction of electronic products, silicon dice are often utilized without encapsulation and mounted directly to the substrate by means of conductive adhesives or BGA mounting. Silicon die often need to be thinned to a few hundred micrometers thickness to fit into compact devices and to reduce parasitics. The intrinsic brittle nature of silicon in combination with the lack of mechanical protection such as encapsulation has made fracture of bare dice a typical failure mechanism in handheld electronic devices. In the current work, we tested to failure {100} silicon dice and obtained mirror–mist boundary measurements for correlation to the fracture strengths of the parts. This work will also present various practical examples of how to reliably conduct failure analysis of fractured silicon dice. The intrinsic brittle nature of silicon in combination with the lack of mechanical protection such as encapsulation has made fracture of bare dice a typical failure mechanism in handheld electronic devices such as cameras, portable computers, tablets, media players, and smart phones. In these products, silicon dice are often utilized without encapsulation and are attached directly to the substrate by means of conductive adhesives or ball grid array mounting. Modern silicon dice used in these products typically have small dimensions and higher flexural strength compared to their predecessors. Prior silicon fractographic findings have investigated low strength failures. In the current work, we extend the quantitative fractography of silicon to the high failure stress regime. We have mechanically tested modern silicon dice to failure by four-point bending and obtained mirror–mist boundary measurements for correlation to the fracture strengths of the specimens. Two key areas are addressed which improve the practical application of quantitative fractography to modern silicon dice: (1) application of silicon fractography to high flexural strength regimes and (2) development of a systematic means of reliably measuring fracture surface features.</p></div>
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Although the utilization of silicon dice in electronic devices has been in place for approximately 50 years, its widespread application has occurred more recently with the rapid expansion of the consumer markets for digital devices such as cameras, personal computers, video players, and smart phones. In particular, due to the recent market drive in the miniaturization and cost reduction of electronic products, silicon dice are often utilized without encapsulation and mounted directly to the substrate by means of conductive adhesives or BGA mounting. Silicon die often need to be thinned to a few hundred micrometers thickness to fit into compact devices and to reduce parasitics. The intrinsic brittle nature of silicon in combination with the lack of mechanical protection such as encapsulation has made fracture of bare dice a typical failure mechanism in handheld electronic devices. In the current work, we tested to failure {100} silicon dice and obtained mirror–mist boundary measurements for correlation to the fracture strengths of the parts. This work will also present various practical examples of how to reliably conduct failure analysis of fractured silicon dice. The intrinsic brittle nature of silicon in combination with the lack of mechanical protection such as encapsulation has made fracture of bare dice a typical failure mechanism in handheld electronic devices such as cameras, portable computers, tablets, media players, and smart phones. In these products, silicon dice are often utilized without encapsulation and are attached directly to the substrate by means of conductive adhesives or ball grid array mounting. Modern silicon dice used in these products typically have small dimensions and higher flexural strength compared to their predecessors. Prior silicon fractographic findings have investigated low strength failures. In the current work, we extend the quantitative fractography of silicon to the high failure stress regime. We have mechanically tested modern silicon dice to failure by four-point bending and obtained mirror–mist boundary measurements for correlation to the fracture strengths of the specimens. Two key areas are addressed which improve the practical application of quantitative fractography to modern silicon dice: (1) application of silicon fractography to high flexural strength regimes and (2) development of a systematic means of reliably measuring fracture surface features.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12087" xmlns="http://purl.org/rss/1.0/"><title>SiSiC Heat Exchangers for Recuperative Gas Burners with Highly Structured Surface Elements</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12087</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">SiSiC Heat Exchangers for Recuperative Gas Burners with Highly Structured Surface Elements</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Alberto Ortona, Dimosthenis Trimis, Sandro Gianella, Paolo Fino, Emmanuel Boulet, Volker Uhlig, Robert Eder, Claire Chazelas, Tobias Grämer, Giuseppe D'Amico, Enrico Cresci, Joachim G. Wünning, Herwig Altena, Franz Beneke, Michel Debier</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-29T10:10:06.725871-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12087</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12087</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12087</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Heat exchangers are used in gas burners as recuperators. Their efficiency is proportional to their surface which is usually limited by the burner length and diameter. Ceramic recuperators used nowadays in industrial burners are tubular. We studied and developed a new generation of ceramic heat exchanger with the final goal of increasing the efficiency or, at similar efficiencies, of reducing their size and weight. A commercial SiSiC heat exchanger component was used to guarantee safety and robustness. The use of structured textile geometries followed by their conversion into a ceramic is the main innovation of this work.</p></div>
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Heat exchangers are used in gas burners as recuperators. Their efficiency is proportional to their surface which is usually limited by the burner length and diameter. Ceramic recuperators used nowadays in industrial burners are tubular. We studied and developed a new generation of ceramic heat exchanger with the final goal of increasing the efficiency or, at similar efficiencies, of reducing their size and weight. A commercial SiSiC heat exchanger component was used to guarantee safety and robustness. The use of structured textile geometries followed by their conversion into a ceramic is the main innovation of this work.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12095" xmlns="http://purl.org/rss/1.0/"><title>Loading and Delivery of Anticancer Drugs using Montmorillonite</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12095</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Loading and Delivery of Anticancer Drugs using Montmorillonite</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Maria Betsiou, Georgios Bantsis, Costas Sikalidis, Ioanna Zoi, Anna Bourliva</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-29T09:59:28.156049-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12095</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12095</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12095</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>This study aimed to investigate <em>in vitro</em> the montmorillonite (MMT) as carrier for gemcitabine hydrochloride (dFdU.HCl) and oxaliplatin (DACH-Pt). The maximum adsorption capacities of MMT and their respective mechanisms were determined through a soaking procedure (387.5 mg dFdU.HCl/g MMT were adsorbed in 32 h, 83 mg DACH-Pt/g MMT in 48 h). Release kinetics studies were carried out soaking the samples of loaded MMT in simulated body fluids (SBF). Finally, in an attempt to explain the mechanism of drug delivery, the chemical interactions were studied theoretically, according to the adsorption and release profiles.</p></div>
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This study aimed to investigate in vitro the montmorillonite (MMT) as carrier for gemcitabine hydrochloride (dFdU.HCl) and oxaliplatin (DACH-Pt). The maximum adsorption capacities of MMT and their respective mechanisms were determined through a soaking procedure (387.5 mg dFdU.HCl/g MMT were adsorbed in 32 h, 83 mg DACH-Pt/g MMT in 48 h). Release kinetics studies were carried out soaking the samples of loaded MMT in simulated body fluids (SBF). Finally, in an attempt to explain the mechanism of drug delivery, the chemical interactions were studied theoretically, according to the adsorption and release profiles.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12092" xmlns="http://purl.org/rss/1.0/"><title>High-Temperature Flexural Strength and Thermal Stability of Near Zero Expanding doped Aluminum Titanate Ceramics for Diesel Particulate Filters Applications</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12092</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">High-Temperature Flexural Strength and Thermal Stability of Near Zero Expanding doped Aluminum Titanate Ceramics for Diesel Particulate Filters Applications</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ramanathan Papitha, Madireddy Buchi Suresh, Das Dibakar, Roy Johnson</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-25T10:12:06.345161-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12092</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12092</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12092</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A substantial increase in sinterability, high-temperature flexural strength, thermal stability in combination with an average thermal expansion of 0.42 × 10<sup>−6</sup>/<sup>°</sup>C (30–1000°C) is achieved through magnesium silicate (Mg<sub>3</sub>Si<sub>4</sub>O<sub>10</sub>(OH)<sub>2</sub>) doping of Aluminum Titanate (Al<sub>2</sub>TiO<sub>5</sub>) ceramics. Doped specimens exhibited the sintered density of 99% of theoretical density at 1550°C and a maximum enhancement of 169.23% (70 MPa) in flexural strength at 1200°C as compared with 26 MPa measured at 30°C. Enhancement of flexural strength at elevated temperature can be attributed to the increasing extent of thermally activated crack blunting with increasing temperature, which is further evident from the dilatometric hysteresis curve recorded for these samples. XRD investigations of undoped (Al<sub>2</sub>TiO<sub>5</sub>, AT) samples annealed at 1100°C for 5 and 10 h have shown clear evidence of decomposition to precursor oxides by 7% and 21.13%, respectively. However, the samples of magnesium silicate–doped Al<sub>2</sub>TiO<sub>5</sub> (TAT) under identical conditions have shown no sign of decomposition, indicating significantly high thermal stability. TAT formulations were also extrusion processed to investigate the suitability of forming cellular honeycomb structures. TAT formulation with superior thermo-mechanical properties and excellent adaptability for extrusion processing can be explored for the development of next generation diesel particulate filters (DPF).</p></div>
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A substantial increase in sinterability, high-temperature flexural strength, thermal stability in combination with an average thermal expansion of 0.42 × 10−6/°C (30–1000°C) is achieved through magnesium silicate (Mg3Si4O10(OH)2) doping of Aluminum Titanate (Al2TiO5) ceramics. Doped specimens exhibited the sintered density of 99% of theoretical density at 1550°C and a maximum enhancement of 169.23% (70 MPa) in flexural strength at 1200°C as compared with 26 MPa measured at 30°C. Enhancement of flexural strength at elevated temperature can be attributed to the increasing extent of thermally activated crack blunting with increasing temperature, which is further evident from the dilatometric hysteresis curve recorded for these samples. XRD investigations of undoped (Al2TiO5, AT) samples annealed at 1100°C for 5 and 10 h have shown clear evidence of decomposition to precursor oxides by 7% and 21.13%, respectively. However, the samples of magnesium silicate–doped Al2TiO5 (TAT) under identical conditions have shown no sign of decomposition, indicating significantly high thermal stability. TAT formulations were also extrusion processed to investigate the suitability of forming cellular honeycomb structures. TAT formulation with superior thermo-mechanical properties and excellent adaptability for extrusion processing can be explored for the development of next generation diesel particulate filters (DPF).
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12062" xmlns="http://purl.org/rss/1.0/"><title>A Novel Way to Prepare Visible-Light-Responsive WO3/TiO2 Composite Film with High Porosity</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12062</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A Novel Way to Prepare Visible-Light-Responsive WO3/TiO2 Composite Film with High Porosity</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Qiang Luo, Qizhou Cai, Jian He, Xinwei Li, Xidi Chen, Zhenhua Pan, Yujie Li</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-25T10:11:56.539811-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12062</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12062</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12062</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Amorphous oxide film was prepared on the titanium substrate by plasma electrolytic oxidation (PEO) technology in acidic electrolyte consisting of tungstate and then subject to calcination in air. Films were characterized by scanning electron microscopy, energy dispersive X-ray, X-ray diffraction, X-ray photoelectron spectroscopy, photoluminescence, and UV-Vis DRS before and after calcination, respectively. Calcined film consisted of anatase and WO<sub>3</sub>, showing more open structure compared with uncalcined film. Furthermore, the absorption edge of calcined film was shifted to visible light region and the recombination of photo-induced carriers was inhibited effectively, resulting that WO<sub>3</sub>/TiO<sub>2</sub> composite film produced by PEO technology and calcination should be effective as a visible-light-responsive photocatalyst.</p></div>
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Amorphous oxide film was prepared on the titanium substrate by plasma electrolytic oxidation (PEO) technology in acidic electrolyte consisting of tungstate and then subject to calcination in air. Films were characterized by scanning electron microscopy, energy dispersive X-ray, X-ray diffraction, X-ray photoelectron spectroscopy, photoluminescence, and UV-Vis DRS before and after calcination, respectively. Calcined film consisted of anatase and WO3, showing more open structure compared with uncalcined film. Furthermore, the absorption edge of calcined film was shifted to visible light region and the recombination of photo-induced carriers was inhibited effectively, resulting that WO3/TiO2 composite film produced by PEO technology and calcination should be effective as a visible-light-responsive photocatalyst.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12046" xmlns="http://purl.org/rss/1.0/"><title>Photocatalytic Efficiency of Zeolite-Based TiO2 Composites for Reduction of Cu (II): Kinetic Models</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12046</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Photocatalytic Efficiency of Zeolite-Based TiO2 Composites for Reduction of Cu (II): Kinetic Models</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Anca Peter, Leonard Mihaly-Cozmuta, Anca Mihaly-Cozmuta, Camelia Nicula, Lucian Barbu Tudoran, Adriana Vulpoi, Lucian Baia</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-25T10:11:26.553745-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12046</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12046</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12046</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>This study evaluates the photoactivity of novel zeolite-based TiO<sub>2</sub> composites modified with metal particles for the photoreduction of Cu<sup>2+</sup>, depending on the zeolite and metal particles (Ag or Fe) content and to establish the photoreduction mechanism. The composites have been prepared by incorporating zeolite particles in the sols during the sol-gel preparation of the TiO<sub>2</sub>, followed by impregnation of the gels in solutions containing metal ions. The zeolite-based TiO<sub>2</sub> composites have been characterized using X-ray diffraction, Raman and FTIR spectroscopy techniques and TEM microscopy. The role of zeolite particles in the photoreduction process was demonstrated by using different kinetic models. The apparent constant rate for photoreduction increases in direct proportion with the content of zeolite and is higher for the composites modified with Fe than for those modified with Ag nanoparticles. The results demonstrate that composites have a higher photocatalytic efficiency than TiO<sub>2</sub>. The experiments in this study reveal that the migration of Cu<sup>2+</sup> in solution occurs rapidly and that the diffusion through the film on the composite's surface and, subsequently, the photoreduction process are the rate limiting steps. The role of the zeolite in photoreduction is to diminish the recombination rate of the charge carriers.</p></div>
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This study evaluates the photoactivity of novel zeolite-based TiO2 composites modified with metal particles for the photoreduction of Cu2+, depending on the zeolite and metal particles (Ag or Fe) content and to establish the photoreduction mechanism. The composites have been prepared by incorporating zeolite particles in the sols during the sol-gel preparation of the TiO2, followed by impregnation of the gels in solutions containing metal ions. The zeolite-based TiO2 composites have been characterized using X-ray diffraction, Raman and FTIR spectroscopy techniques and TEM microscopy. The role of zeolite particles in the photoreduction process was demonstrated by using different kinetic models. The apparent constant rate for photoreduction increases in direct proportion with the content of zeolite and is higher for the composites modified with Fe than for those modified with Ag nanoparticles. The results demonstrate that composites have a higher photocatalytic efficiency than TiO2. The experiments in this study reveal that the migration of Cu2+ in solution occurs rapidly and that the diffusion through the film on the composite's surface and, subsequently, the photoreduction process are the rate limiting steps. The role of the zeolite in photoreduction is to diminish the recombination rate of the charge carriers.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12106" xmlns="http://purl.org/rss/1.0/"><title>SrLn2Al2O7 (Ln = La, Nd, Sm) Microwave Dielectric Ceramic New Materials</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12106</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">SrLn2Al2O7 (Ln = La, Nd, Sm) Microwave Dielectric Ceramic New Materials</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Lei Yi, Xiao Qiang Liu, Lei Li, Xiang Ming Chen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-24T09:40:15.744322-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12106</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12106</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12106</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>SrLn<sub>2</sub>Al<sub>2</sub>O<sub>7</sub> (Ln = La, Nd, Sm) ceramics were proposed and investigated as new candidates for ultra-low loss microwave dielectric materials. These ceramics indicated the Ruddlesden–Popper structure of general formula A<sub><em>n</em>+1</sub>B<sub><em>n</em></sub>O<sub>3<em>n</em>+1</sub> with <em>n</em> = 2, which was composed by <em>n</em> perovskite layers alternating with one rock-salt layer. Very high <em>Qf</em> value combined with a dielectric constant around 20 was obtained in the present ceramics, where the near-zero temperature coefficient of resonant frequency varied from negative to positive with changing Ln from La to Sm. The best combination of microwave dielectric characteristics was obtained as the following: <em>ε</em><sub><em>r</em></sub> = 18.2, <em>Qf </em>= 71,680 GHz, and <em>τ</em><sub><em>f</em></sub> = −22.1 ppm/°C for SrLa<sub>2</sub>Al<sub>2</sub>O<sub>7</sub>; <em>ε</em><sub><em>r</em></sub> = 20.5, <em>Qf</em> = 65,500 GHz, and <em>τ</em><sub><em>f</em></sub> = −4.3 ppm/°C for SrNd<sub>2</sub>Al<sub>2</sub>O<sub>7</sub>; and <em>ε</em><sub><em>r</em></sub> = 21.6, <em>Qf</em> = 64,680 GHz, and <em>τ</em><sub><em>f</em></sub> = +4.0 ppm/°C for SrSm<sub>2</sub>Al<sub>2</sub>O<sub>7</sub>.</p></div>
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SrLn2Al2O7 (Ln = La, Nd, Sm) ceramics were proposed and investigated as new candidates for ultra-low loss microwave dielectric materials. These ceramics indicated the Ruddlesden–Popper structure of general formula An+1BnO3n+1 with n = 2, which was composed by n perovskite layers alternating with one rock-salt layer. Very high Qf value combined with a dielectric constant around 20 was obtained in the present ceramics, where the near-zero temperature coefficient of resonant frequency varied from negative to positive with changing Ln from La to Sm. The best combination of microwave dielectric characteristics was obtained as the following: εr = 18.2, Qf = 71,680 GHz, and τf = −22.1 ppm/°C for SrLa2Al2O7; εr = 20.5, Qf = 65,500 GHz, and τf = −4.3 ppm/°C for SrNd2Al2O7; and εr = 21.6, Qf = 64,680 GHz, and τf = +4.0 ppm/°C for SrSm2Al2O7.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12086" xmlns="http://purl.org/rss/1.0/"><title>Immobilization of TiO2 into Self-Supporting Photocatalytic Foam: Influence of Calcination Temperature</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12086</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Immobilization of TiO2 into Self-Supporting Photocatalytic Foam: Influence of Calcination Temperature</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Tom Tytgat, Marianne Smits, Silvia Lenaerts, Sammy W. Verbruggen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-24T09:39:56.916738-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12086</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12086</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12086</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Immobilization of photocatalytic powder is crucial to obtain industrially relevant purification processes. To achieve this goal, self-supporting TiO<sub>2</sub> foams were manufactured by a polyacrylamide gel process. These gels were calcined at different temperatures to study the effect of the calcination temperature on foam characteristics (rigidity, crystallinity, and porosity) and its influence on photocatalytic activity. The results show that an optimal degradation is achieved for those foams calcined between 700 and 800°C. Calcination at higher temperatures results in a steep decrease in activity, explained by stability issues of the material due to formation of Na<sub>2</sub>SO<sub>4</sub> phases and a larger rutile fraction.</p></div>
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Immobilization of photocatalytic powder is crucial to obtain industrially relevant purification processes. To achieve this goal, self-supporting TiO2 foams were manufactured by a polyacrylamide gel process. These gels were calcined at different temperatures to study the effect of the calcination temperature on foam characteristics (rigidity, crystallinity, and porosity) and its influence on photocatalytic activity. The results show that an optimal degradation is achieved for those foams calcined between 700 and 800°C. Calcination at higher temperatures results in a steep decrease in activity, explained by stability issues of the material due to formation of Na2SO4 phases and a larger rutile fraction.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12105" xmlns="http://purl.org/rss/1.0/"><title>Effect of Particle Size on the Optical Properties of Yellow Silicate Phosphor in Light-Emitting Diodes</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12105</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of Particle Size on the Optical Properties of Yellow Silicate Phosphor in Light-Emitting Diodes</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Min-Suk Jang, Wan-Ho Kim, Young-Rae Kang, Sang-Bin Song, Jae-Pil Kim, Jin-Hyeok Kim</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-23T11:57:14.42757-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12105</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12105</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12105</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Understanding the effect of particle size on the optical properties of phosphor is important to increase packaging efficiency in white light-emitting diodes (LEDs). We have investigated the effect of particle size (10–20 μm, 20–25 μm, 25–32 μm) on the optical properties of a yellow silicate phosphor adopted in white LEDs. X-ray diffraction results show negligible modification in crystallinity as the particle size of the yellow silicate phosphor varies, whereas the photoluminescence excitation intensity and quantum yield are enhanced as the particle size increased. LED packages fabricated using phosphors with different mean particle sizes, and their optical properties were analyzed. The radiant flux improved with increasing particle size, whereas the luminous flux increased with decreasing particle size. The effect of immersion on the optical properties of the LED light source has been also measured, and the details are discussed.</p></div>
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Understanding the effect of particle size on the optical properties of phosphor is important to increase packaging efficiency in white light-emitting diodes (LEDs). We have investigated the effect of particle size (10–20 μm, 20–25 μm, 25–32 μm) on the optical properties of a yellow silicate phosphor adopted in white LEDs. X-ray diffraction results show negligible modification in crystallinity as the particle size of the yellow silicate phosphor varies, whereas the photoluminescence excitation intensity and quantum yield are enhanced as the particle size increased. LED packages fabricated using phosphors with different mean particle sizes, and their optical properties were analyzed. The radiant flux improved with increasing particle size, whereas the luminous flux increased with decreasing particle size. The effect of immersion on the optical properties of the LED light source has been also measured, and the details are discussed.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12091" xmlns="http://purl.org/rss/1.0/"><title>Effects of Particle Size on Electromagnetic and Microwave Absorption Properties of La0.7Sr0.3MnO3±δ-Epoxy Composite</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12091</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effects of Particle Size on Electromagnetic and Microwave Absorption Properties of La0.7Sr0.3MnO3±δ-Epoxy Composite</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Shuyuan Zhang, Quanxi Cao, Maolin Zhang, Lei Cai, Qidong Yan</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-23T11:56:35.946399-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12091</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12091</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12091</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>La<sub>0.7</sub>Sr<sub>0.3</sub>MnO<sub>3±δ</sub> powders were fabricated by solid-state reaction method at 1473 K for 4 h. The precursors were prepared by ball-milling raw materials for 3, 6, 9, and 12 h, respectively. The crystal structures, particle size, and morphologies of precursors and prepared La<sub>0.7</sub>Sr<sub>0.3</sub>MnO<sub>3±δ</sub> were characterized by XRD, laser particle size analyzer and SEM, respectively. It is found that La<sub>0.7</sub>Sr<sub>0.3</sub>MnO<sub>3±δ</sub> possessed large particle size by ball-milling raw materials for a long time. Results indicated that La<sub>0.7</sub>Sr<sub>0.3</sub>MnO<sub>3±δ</sub>, synthesized by ball-milling raw materials for 3 h, exhibited the optimal microwave absorption properties. The maximum reflection loss was −28.8 dB, and the −6 dB absorption bandwidth was 5.80 GHz.</p></div>
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La0.7Sr0.3MnO3±δ powders were fabricated by solid-state reaction method at 1473 K for 4 h. The precursors were prepared by ball-milling raw materials for 3, 6, 9, and 12 h, respectively. The crystal structures, particle size, and morphologies of precursors and prepared La0.7Sr0.3MnO3±δ were characterized by XRD, laser particle size analyzer and SEM, respectively. It is found that La0.7Sr0.3MnO3±δ possessed large particle size by ball-milling raw materials for a long time. Results indicated that La0.7Sr0.3MnO3±δ, synthesized by ball-milling raw materials for 3 h, exhibited the optimal microwave absorption properties. The maximum reflection loss was −28.8 dB, and the −6 dB absorption bandwidth was 5.80 GHz.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12060" xmlns="http://purl.org/rss/1.0/"><title>Texture, Microstructure, and Tribological Behavior in TiAlN/SiNx Multilayers</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12060</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Texture, Microstructure, and Tribological Behavior in TiAlN/SiNx Multilayers</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yu-Chen Chan, Hsien-Wei Chen, Jenq-Gong Duh, Jyh-Wei Lee</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-23T11:56:32.44491-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12060</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12060</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12060</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>TiAlN/SiN<sub>x</sub> multilayers were fabricated by RF reactive magnetron sputtering. Characterizations by TEM, dark-field images, and SEM revealed the dependence for the thickness of SiN<sub>x</sub> (<em>l</em><sub>SiNx</sub>) on the texture and microstructure evolution in multilayers. Epitaxial stabilization in multilayer ameliorated the hardness and H/E ratio. With increasing the <em>l</em><sub>SiNx</sub>, the amorphous SiN<sub>x</sub> altered the coherent interfaces and the superlattice structure, leading to an appreciable decrease in hardness. Nevertheless, this fine-grained coating exhibited superior resistance to plastic deformation. In the ball-on-disk wear tests, the observation of coefficient of friction, worn surfaces, and cross-sectional worn scars verified that multilayers showed better tribological resistance than that of TiAlN monolayer. Two antiwear mechanisms on the basis of hardness variation and microstructure evolution were proposed to elucidate the favorable durability of TiAlN/SiN<sub>x</sub> multilayers with various <em>l</em><sub>SiNx</sub>.</p></div>
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TiAlN/SiNx multilayers were fabricated by RF reactive magnetron sputtering. Characterizations by TEM, dark-field images, and SEM revealed the dependence for the thickness of SiNx (lSiNx) on the texture and microstructure evolution in multilayers. Epitaxial stabilization in multilayer ameliorated the hardness and H/E ratio. With increasing the lSiNx, the amorphous SiNx altered the coherent interfaces and the superlattice structure, leading to an appreciable decrease in hardness. Nevertheless, this fine-grained coating exhibited superior resistance to plastic deformation. In the ball-on-disk wear tests, the observation of coefficient of friction, worn surfaces, and cross-sectional worn scars verified that multilayers showed better tribological resistance than that of TiAlN monolayer. Two antiwear mechanisms on the basis of hardness variation and microstructure evolution were proposed to elucidate the favorable durability of TiAlN/SiNx multilayers with various lSiNx.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12061" xmlns="http://purl.org/rss/1.0/"><title>Microstructure and Anisotropic Properties of Textured ZrB2 and ZrB2–MoSi2 Ceramics Prepared by Strong Magnetic Field Alignment</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12061</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Microstructure and Anisotropic Properties of Textured ZrB2 and ZrB2–MoSi2 Ceramics Prepared by Strong Magnetic Field Alignment</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Wen-Wen Wu, Yoshio Sakka, Tohru S. Suzuki, Guo-Jun Zhang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-23T11:50:40.310303-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12061</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12061</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12061</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Dense, highly textured ZrB<sub>2</sub> and ZrB<sub>2</sub>–MoSi<sub>2</sub> ceramics were fabricated via a strong magnetic field alignment method followed by spark plasma sintering. Unlike with the previous studies, which only focused on the alignment of single-phase particles, both ZrB<sub>2</sub> and MoSi<sub>2</sub>, which exhibited a magnetic anisotropy, have been aligned in this study. The alignment of MoSi<sub>2</sub> in the same direction of ZrB<sub>2</sub> enhanced the degree of orientation of ZrB<sub>2</sub>, decreased the grain size, but increased the aspect ratio of the platelet ZrB<sub>2</sub> grains. The microstructure and anisotropic mechanical properties as well as the oxidation resistance in different directions were discussed.</p></div>
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Dense, highly textured ZrB2 and ZrB2–MoSi2 ceramics were fabricated via a strong magnetic field alignment method followed by spark plasma sintering. Unlike with the previous studies, which only focused on the alignment of single-phase particles, both ZrB2 and MoSi2, which exhibited a magnetic anisotropy, have been aligned in this study. The alignment of MoSi2 in the same direction of ZrB2 enhanced the degree of orientation of ZrB2, decreased the grain size, but increased the aspect ratio of the platelet ZrB2 grains. The microstructure and anisotropic mechanical properties as well as the oxidation resistance in different directions were discussed.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12070" xmlns="http://purl.org/rss/1.0/"><title>Synthesis and Properties of a New Dental Material Based on Nano-Structured Highly Active Calcium Silicates and Calcium Carbonates</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12070</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Synthesis and Properties of a New Dental Material Based on Nano-Structured Highly Active Calcium Silicates and Calcium Carbonates</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Vukoman Jokanović, Božana Čolović, Miodrag Mitrić, Dejan Marković, Bojana Ćetenović</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-23T11:50:30.656988-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12070</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12070</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12070</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A synthesis of a new dental material, based on nano-structured highly active calcium silicates and calcium carbonates, is described in this paper. Phase analysis of this material, before and after hydration, was performed by X-ray diffraction and showed that active silicate phases were transformed into tobermorite phase, while carbonates remained unchanged. The mechanism of hydration was fully described. The morphology of the sample was studied by SEM, and typical appearance of the present phases was particularly discussed. The mechanical properties and setting time of this material make it very promising for potential application in dental practice.</p></div>
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A synthesis of a new dental material, based on nano-structured highly active calcium silicates and calcium carbonates, is described in this paper. Phase analysis of this material, before and after hydration, was performed by X-ray diffraction and showed that active silicate phases were transformed into tobermorite phase, while carbonates remained unchanged. The mechanism of hydration was fully described. The morphology of the sample was studied by SEM, and typical appearance of the present phases was particularly discussed. The mechanical properties and setting time of this material make it very promising for potential application in dental practice.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12083" xmlns="http://purl.org/rss/1.0/"><title>Sustainable Infrastructure Materials: Challenges and Opportunities</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12083</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Sustainable Infrastructure Materials: Challenges and Opportunities</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mohammad Pour-Ghaz</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-23T10:10:51.179044-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12083</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12083</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12083</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The recent quest for developing new low carbon footprint construction materials to lower the environmental emissions and implications of infrastructure has imposed many challenges and has created many opportunities for research and development in academia and industrial sectors. The present paper, discusses and summaries these challenges and opportunities and provides a synopsis of the ideas presented in the Infrastructure sessions of the Fourth International Congress on Ceramics (ICC4). This paper also discusses recent advances in the development of sustainable infrastructure materials.</p></div>
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The recent quest for developing new low carbon footprint construction materials to lower the environmental emissions and implications of infrastructure has imposed many challenges and has created many opportunities for research and development in academia and industrial sectors. The present paper, discusses and summaries these challenges and opportunities and provides a synopsis of the ideas presented in the Infrastructure sessions of the Fourth International Congress on Ceramics (ICC4). This paper also discusses recent advances in the development of sustainable infrastructure materials.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12099" xmlns="http://purl.org/rss/1.0/"><title>New Alumina-Based Novel Ceramic Nanopigments: An Alternative to the Purple of Cassius</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12099</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">New Alumina-Based Novel Ceramic Nanopigments: An Alternative to the Purple of Cassius</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Agnieszka Maria Jastrzębska, Patrycja Kurtycz, Andrzej Roman Olszyna, Joanna Jureczko, Antoni Ryszard Kunicki</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-23T10:10:33.405886-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12099</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12099</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12099</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The present article presents first comparative study on three different dry solgel methods of producing new alumina-based dark violet, light pink ceramic nanopigments as well as ruby-red ceramic nanopigment — an alternative to the Purple of Cassius. Gold nanoparticles are built directly on a carrier of an aluminum oxide nanopowder, which finally yields Al<sub>2</sub>O<sub>3</sub>/Au nanopowders possessing colors ranging from light pink to light violet as well as ruby-red.</p></div>
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The present article presents first comparative study on three different dry solgel methods of producing new alumina-based dark violet, light pink ceramic nanopigments as well as ruby-red ceramic nanopigment — an alternative to the Purple of Cassius. Gold nanoparticles are built directly on a carrier of an aluminum oxide nanopowder, which finally yields Al2O3/Au nanopowders possessing colors ranging from light pink to light violet as well as ruby-red.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12107" xmlns="http://purl.org/rss/1.0/"><title>Correlation between Sn substitution for Ti and Microwave Dielectric Properties of Magnesium Titanate Ceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12107</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Correlation between Sn substitution for Ti and Microwave Dielectric Properties of Magnesium Titanate Ceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hongtao Yu, Xiaomei Xue, Guangliang Xu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-19T11:05:26.59385-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12107</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12107</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12107</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The relationship between Sn substitution for Ti and microwave dielectric properties of Mg(Ti<sub>1-<em>x</em></sub>Sn<sub><em>x</em></sub>)O<sub>3</sub> ceramics was investigated. Sn<sup>4+</sup> could substitute for Ti<sup>4+</sup> in MgTiO<sub>3</sub> and increase the crystal volume. All samples exhibited the MgTiO<sub>3</sub>-type phase with ilmenite structure as main phase. At the x range from 0 to 0.05, the secondary phase of Mg<sub>2</sub>TiO<sub>5</sub> was observed. Upon further increasing Sn content up to 0.15, the SnO<sub>2</sub> phase appeared. When the <em>x</em> value increased from 0 to 0.05, the dielectric constant decreased slightly and the quality factor increased sharply, whereas the dielectric constant increased and the quality factor decreased as the <em>x</em> value varied from 0.05 to 0.15. The temperature coefficient of resonant frequency moved toward positive value with Sn substitution. In particular, at the x range from 0.05 to 0.07, the ceramic sintered at 1360°C for 4 h exhibited excellent microwave dielectric properties of <em>ε</em><sub>r</sub> = 16.8–17.1, <em>Q</em><sub>f</sub> = 298,000–312,000 and <em>τ</em><sub>f</sub> = −53~−50 ppm/°C.</p></div>
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The relationship between Sn substitution for Ti and microwave dielectric properties of Mg(Ti1-xSnx)O3 ceramics was investigated. Sn4+ could substitute for Ti4+ in MgTiO3 and increase the crystal volume. All samples exhibited the MgTiO3-type phase with ilmenite structure as main phase. At the x range from 0 to 0.05, the secondary phase of Mg2TiO5 was observed. Upon further increasing Sn content up to 0.15, the SnO2 phase appeared. When the x value increased from 0 to 0.05, the dielectric constant decreased slightly and the quality factor increased sharply, whereas the dielectric constant increased and the quality factor decreased as the x value varied from 0.05 to 0.15. The temperature coefficient of resonant frequency moved toward positive value with Sn substitution. In particular, at the x range from 0.05 to 0.07, the ceramic sintered at 1360°C for 4 h exhibited excellent microwave dielectric properties of εr = 16.8–17.1, Qf = 298,000–312,000 and τf = −53~−50 ppm/°C.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12102" xmlns="http://purl.org/rss/1.0/"><title>Dielectric Properties of Boron Nitride in THz Region Synthesized with Nonenergetic CVD</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12102</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Dielectric Properties of Boron Nitride in THz Region Synthesized with Nonenergetic CVD</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Marián Janek, Andrej Vincze, Juraj Darmo, Vojtech Szöcs, Marián Matejdes, Tomáš Zacher, Štefan Kavecký, Vladimír Danielik, Dusan Velič, Dušan Lorenc, Rudolf Srnánek, Alexander Šatka, Daniel Haško, Jozef Matuška, František Uherek</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-19T11:05:22.782305-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12102</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12102</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12102</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Pyrolytic boron nitride (pBN) was prepared with a nonenergetic chemical vapor deposition. Two tests were performed (i) short time deposition to investigate rate and volume deposition of injected reaction gases and (ii) long time deposition to characterize possible qualitative differences of the formed BN layer. SEM, XRD, FTIR, Raman spectroscopy, and Terahertz time-domain spectroscopy proved that there are small qualitative differences in the pBN deposited at various distances from the blast pipe. The quality of the phase synthesized was resolved with highly sensitive THz-TDS technique, the index of refraction <em>n</em><sub>pBN</sub> varied at 2.0 THz (66.6 cm) from 2.018 ± 0.003 to 2.124 ± 0.005.</p></div>
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Pyrolytic boron nitride (pBN) was prepared with a nonenergetic chemical vapor deposition. Two tests were performed (i) short time deposition to investigate rate and volume deposition of injected reaction gases and (ii) long time deposition to characterize possible qualitative differences of the formed BN layer. SEM, XRD, FTIR, Raman spectroscopy, and Terahertz time-domain spectroscopy proved that there are small qualitative differences in the pBN deposited at various distances from the blast pipe. The quality of the phase synthesized was resolved with highly sensitive THz-TDS technique, the index of refraction npBN varied at 2.0 THz (66.6 cm) from 2.018 ± 0.003 to 2.124 ± 0.005.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12097" xmlns="http://purl.org/rss/1.0/"><title>In situ TiC Ceramic Particles Locally Reinforced Al-Si Matrix Composites Prepared by SHS-Casting Method from the Al-Si-Ti-C System</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12097</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">In situ TiC Ceramic Particles Locally Reinforced Al-Si Matrix Composites Prepared by SHS-Casting Method from the Al-Si-Ti-C System</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mengxian Zhang, Yanqiu Huo, Li Ma, Bin Huang, Qiaodan Hu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-18T10:03:07.083102-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12097</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12097</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12097</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Using Al-Si-Ti-C powder mixtures, TiC grains locally reinforced Al-Si matrix composites were produced through self-propagating high-temperature synthesis and casting method. The formation of TiC could be ascribed to the dissolution–reaction–precipitation mechanism. The TiC grains were uniformly distributed in the locally reinforced regions of the Al-Si matrix. With increasing Al-Si content, the size of TiC grains decreased. No pores and cracks were present at the interface between the Al-Si matrix and the reinforced regions. Wear resistance of the locally reinforced regions is significantly improved compared with that of the Al-Si matrix.</p></div>
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Using Al-Si-Ti-C powder mixtures, TiC grains locally reinforced Al-Si matrix composites were produced through self-propagating high-temperature synthesis and casting method. The formation of TiC could be ascribed to the dissolution–reaction–precipitation mechanism. The TiC grains were uniformly distributed in the locally reinforced regions of the Al-Si matrix. With increasing Al-Si content, the size of TiC grains decreased. No pores and cracks were present at the interface between the Al-Si matrix and the reinforced regions. Wear resistance of the locally reinforced regions is significantly improved compared with that of the Al-Si matrix.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02823.x" xmlns="http://purl.org/rss/1.0/"><title>Structural and Microwave Dielectric Properties of Mg2TiO4 Ceramics Synthesized by Mechanical Method</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02823.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Structural and Microwave Dielectric Properties of Mg2TiO4 Ceramics Synthesized by Mechanical Method</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ranjan K. Bhuyan, Thatikonda S. Kumar, Dobbidi Pamu, Ajit R. James</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-18T10:02:59.62212-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02823.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02823.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02823.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Low loss <span class="fixed-roman">Mg</span><sub>2</sub><span class="fixed-roman">TiO</span><sub>4</sub> (<span class="fixed-roman">MTO</span>) ceramics have been synthesized by mechanical synthesis method. The effect of processing parameters, on initial particle size, microstructure, relative density, and microwave dielectric properties of <span class="fixed-roman">MTO</span> ceramics are investigated. The maximum relative density was obtained 97.75%, and uniform microstructure is observed for the sample sintered at 1325°C for 3 h. The driving force for the sintering can be attributed to the surface energy of fine powders and their defect energy. There is not much variation in dielectric constant (ε<sub>r</sub>) where as <em>Q × f</em><sub><em>o</em></sub> is affected and the values of <em>Q × f</em><sub><em>o</em></sub> are in the range of 99,500–155,500.</p></div>
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Low loss Mg2TiO4 (MTO) ceramics have been synthesized by mechanical synthesis method. The effect of processing parameters, on initial particle size, microstructure, relative density, and microwave dielectric properties of MTO ceramics are investigated. The maximum relative density was obtained 97.75%, and uniform microstructure is observed for the sample sintered at 1325°C for 3 h. The driving force for the sintering can be attributed to the surface energy of fine powders and their defect energy. There is not much variation in dielectric constant (εr) where as Q × fo is affected and the values of Q × fo are in the range of 99,500–155,500.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.02725.x" xmlns="http://purl.org/rss/1.0/"><title>Factors Influencing the Thermal Stability and Lead Sorption Capacity of Hydroxyapatite Manufactured by Precipitation Method Using Industrial Calcium Hydroxide</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.02725.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Factors Influencing the Thermal Stability and Lead Sorption Capacity of Hydroxyapatite Manufactured by Precipitation Method Using Industrial Calcium Hydroxide</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Amin Salem, Elmira Velayi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-18T10:02:50.421575-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.02725.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.02725.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.02725.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>In this study, the thermal stability of hydroxyapatite was investigated as a function of synthesis factors such as pH, aging time, and calcination temperature. Hydroxyapatite was prepared using calcium hydroxide and orthophosphoric acid and the effect of heat treatment on lead sorption were determined by the batch equilibrium technique. Although the thermal stability of powders was independent from the synthesized condition up to 800°C the material produced at neutral pH and aged during 24 h indicated the suitable stability even at 1000°C. Also, the powder synthesized at above condition completely removed lead compared to that for the other powders.</p></div>
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In this study, the thermal stability of hydroxyapatite was investigated as a function of synthesis factors such as pH, aging time, and calcination temperature. Hydroxyapatite was prepared using calcium hydroxide and orthophosphoric acid and the effect of heat treatment on lead sorption were determined by the batch equilibrium technique. Although the thermal stability of powders was independent from the synthesized condition up to 800°C the material produced at neutral pH and aged during 24 h indicated the suitable stability even at 1000°C. Also, the powder synthesized at above condition completely removed lead compared to that for the other powders.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02840.x" xmlns="http://purl.org/rss/1.0/"><title>Nano-Hydroxyapatite Improves the Properties of β-tricalcium Phosphate Bone Scaffolds</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02840.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Nano-Hydroxyapatite Improves the Properties of β-tricalcium Phosphate Bone Scaffolds</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Cijun Shuai, Pei Feng, Yi Nie, Huanglong Hu, Jinglin Liu, Shuping Peng</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-16T10:56:27.711244-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02840.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02840.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02840.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>β-Tricalcium phosphates have been widely used as biomaterials for bone substitutes; however, the poor mechanical properties limit the application in bearing loading bones. In this study, nano-hydroxyapatite has been introduced to improve the mechanical properties for porous bioceramic scaffolds. Nanocomposites containing 0–10 wt% needle-like nano-hydroxyapatite were prepared for investigation. It has been found that needle-like nano-hydroxyapatite improves the toughness, hardness, and compressive strength of the porous β-tricalcium phosphates scaffolds, as well as the microstructure properties. The study provides a reference for the development of safe, excellent bone scaffolds for bone tissue engineering.</p></div>
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β-Tricalcium phosphates have been widely used as biomaterials for bone substitutes; however, the poor mechanical properties limit the application in bearing loading bones. In this study, nano-hydroxyapatite has been introduced to improve the mechanical properties for porous bioceramic scaffolds. Nanocomposites containing 0–10 wt% needle-like nano-hydroxyapatite were prepared for investigation. It has been found that needle-like nano-hydroxyapatite improves the toughness, hardness, and compressive strength of the porous β-tricalcium phosphates scaffolds, as well as the microstructure properties. The study provides a reference for the development of safe, excellent bone scaffolds for bone tissue engineering.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12103" xmlns="http://purl.org/rss/1.0/"><title>Residual Stress Distribution and Characterization on Multi-Curved Armor Tiles</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12103</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Residual Stress Distribution and Characterization on Multi-Curved Armor Tiles</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Liang Wang, Keyu Li, Brian Munn, Virginia Halls, James Zheng</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-16T10:07:18.263547-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12103</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12103</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12103</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Residual stresses were measured on numerous multi-curved, ballistic tiles made from either silicon carbide or boron carbide. Residual stresses were measured at 155 locations to determine what affect parameters such as material, material processing, tile geometry, and manufacturer had on residual stress type and magnitude. 23% of data points had tensile residual stress. The highest residual stresses were measured in tiles with either the largest surface area or smallest plate thickness. Higher stresses were measured in silicon carbide tiles compared with boron carbide tiles. Residual stresses in tiles consolidated by hot pressing measured on average 10 MPa higher than those by pressureless sintering.</p></div>
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Residual stresses were measured on numerous multi-curved, ballistic tiles made from either silicon carbide or boron carbide. Residual stresses were measured at 155 locations to determine what affect parameters such as material, material processing, tile geometry, and manufacturer had on residual stress type and magnitude. 23% of data points had tensile residual stress. The highest residual stresses were measured in tiles with either the largest surface area or smallest plate thickness. Higher stresses were measured in silicon carbide tiles compared with boron carbide tiles. Residual stresses in tiles consolidated by hot pressing measured on average 10 MPa higher than those by pressureless sintering.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12104" xmlns="http://purl.org/rss/1.0/"><title>Preparation and Property of Solid-Solution Cu(In,Ga)Se2-Cu2ZnSnSe4 Films Obtained from the Paste Printing of Nanosized Cermet Pastes and Subsequent Selenization</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12104</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Preparation and Property of Solid-Solution Cu(In,Ga)Se2-Cu2ZnSnSe4 Films Obtained from the Paste Printing of Nanosized Cermet Pastes and Subsequent Selenization</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dong-Hau Kuo, Jian-Jhih Chen, Wei-Liang Chen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-16T10:07:11.962193-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12104</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12104</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12104</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="ijac12104-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p>Cu-deficient Cu[(In,Ga)(Zn,Sn)]Se<sub>2</sub> (CIGZTSe) films with the expected composition of 60% Cu(In,Ga)Se<sub>2</sub> (CIGSe) and 20% Cu<sub>2</sub>ZnSnSe<sub>4</sub> (CZTSe) were prepared by paste printing of cermet nanopowder and selenization at 550–650°C for 1 h. The cermet powder contained metallic Cu, Zn, and Sn and ceramic In<sub>2</sub>Se<sub>3,</sub> and Ga<sub>2</sub>Se<sub>3</sub> nanopowders. The CIGZTSe films were single phase and had dense and larger grain size of 1–3 μm. Composition analyses of this CIGZTSe films were executed to demonstrate the defect behavior and the variations of electrical properties with selenization temperature. Our solar cell device made with this film as absorption layer showed power conversion efficiency of 0.86%.</p></div></div>
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Cu-deficient Cu[(In,Ga)(Zn,Sn)]Se2 (CIGZTSe) films with the expected composition of 60% Cu(In,Ga)Se2 (CIGSe) and 20% Cu2ZnSnSe4 (CZTSe) were prepared by paste printing of cermet nanopowder and selenization at 550–650°C for 1 h. The cermet powder contained metallic Cu, Zn, and Sn and ceramic In2Se3, and Ga2Se3 nanopowders. The CIGZTSe films were single phase and had dense and larger grain size of 1–3 μm. Composition analyses of this CIGZTSe films were executed to demonstrate the defect behavior and the variations of electrical properties with selenization temperature. Our solar cell device made with this film as absorption layer showed power conversion efficiency of 0.86%.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12096" xmlns="http://purl.org/rss/1.0/"><title>Combinatorial Composition Films and Dielectric Properties of BaxSr1-xTiO3 Grown on Two-Inch p-Si using PLD Process</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12096</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Combinatorial Composition Films and Dielectric Properties of BaxSr1-xTiO3 Grown on Two-Inch p-Si using PLD Process</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ibrahim M. Abdel-Motaleb, Praveen Navuduri, Young-Zo Yoo, Omar Chmaissem, Jeong-Hwan Song</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-12T14:06:53.43622-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12096</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12096</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12096</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Combinatorial composition films of Ba<sub>x</sub>Sr<sub>1-</sub><sub>x</sub>TiO<sub>3</sub> were grown on two-inch <em>p</em>-Si by pulsed laser deposition. Large areas of six different combinatorial composition films were grown on the same wafer using three primary target materials. Consequently, the deposition of Ba<sub>0.5</sub>Sr<sub>0.5</sub>TiO<sub>3</sub> films was obtained from targets BaTiO<sub>3</sub> and SrTiO<sub>3</sub>, the deposition of Ba<sub>0.3</sub>Sr<sub>0.7</sub>TiO<sub>3</sub> films was obtained from targets SrTiO<sub>3</sub> and Ba<sub>0.6</sub>Sr<sub>0.4</sub>TiO<sub>3</sub>, and the Ba<sub>0.8</sub>Sr<sub>0.2</sub>TiO<sub>3</sub> film was obtained from targets Ba<sub>0.6</sub>Sr<sub>0.4</sub>TiO<sub>3</sub> and BaTiO<sub>3</sub>. The results indicate that the deposited materials are perovskite structures with high dielectric constants ranging from 49.4 to 193.2 and leakage current densities as low as 1.25 × 10<sup>−7 </sup>A/cm<sup>2</sup> at −2V.</p></div>
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Combinatorial composition films of BaxSr1-xTiO3 were grown on two-inch p-Si by pulsed laser deposition. Large areas of six different combinatorial composition films were grown on the same wafer using three primary target materials. Consequently, the deposition of Ba0.5Sr0.5TiO3 films was obtained from targets BaTiO3 and SrTiO3, the deposition of Ba0.3Sr0.7TiO3 films was obtained from targets SrTiO3 and Ba0.6Sr0.4TiO3, and the Ba0.8Sr0.2TiO3 film was obtained from targets Ba0.6Sr0.4TiO3 and BaTiO3. The results indicate that the deposited materials are perovskite structures with high dielectric constants ranging from 49.4 to 193.2 and leakage current densities as low as 1.25 × 10−7 A/cm2 at −2V.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12100" xmlns="http://purl.org/rss/1.0/"><title>Tailoring Carbon Fiber/Carbon Nanotubes Interface to Optimize Mechanical Properties of Cf-CNTs/SiC Composites</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12100</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Tailoring Carbon Fiber/Carbon Nanotubes Interface to Optimize Mechanical Properties of Cf-CNTs/SiC Composites</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jianbao Hu, Shaoming Dong, Bin Wu, Xiangyu Zhang, Haijun Zhou, Zhen Wang, Yanmei Kan</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-12T14:06:43.468249-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12100</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12100</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12100</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>C<sub>f</sub>/SiC composites were fabricated using fiber coatings including CNTs and matrix infiltration using the polymer impregnation and pyrolysis process. Interface between fiber and CNTs (CF/CNTs) was tailored to optimize mechanical properties of hybrid composites. The tailored interphases, such as Pyrocarbon (PyC) and PyC/SiC, protect fibers from degradation during the growth of CNTs successfully. Hybrid composites with well-tailored CF/CNTs interface displayed significantly increased mechanical strength (352 ± 21 MPa) compared with that (34 ± 3 MPa) of composites reinforced with CNTs, which grown on carbon fibers directly. The interfacial bonding strength of hybrid composites was improved and optimized by tailoring the CF/CNTs interface. Interfacial failure modes were studied, and a firm interface bonding at the joint where CNTs grown was observed.</p></div>
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Cf/SiC composites were fabricated using fiber coatings including CNTs and matrix infiltration using the polymer impregnation and pyrolysis process. Interface between fiber and CNTs (CF/CNTs) was tailored to optimize mechanical properties of hybrid composites. The tailored interphases, such as Pyrocarbon (PyC) and PyC/SiC, protect fibers from degradation during the growth of CNTs successfully. Hybrid composites with well-tailored CF/CNTs interface displayed significantly increased mechanical strength (352 ± 21 MPa) compared with that (34 ± 3 MPa) of composites reinforced with CNTs, which grown on carbon fibers directly. The interfacial bonding strength of hybrid composites was improved and optimized by tailoring the CF/CNTs interface. Interfacial failure modes were studied, and a firm interface bonding at the joint where CNTs grown was observed.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12098" xmlns="http://purl.org/rss/1.0/"><title>Lateral Conduction Switching in Sputtered Ni-rich NiO Thin Films for Write-Once-Read-Many-Times Memory Applications</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12098</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Lateral Conduction Switching in Sputtered Ni-rich NiO Thin Films for Write-Once-Read-Many-Times Memory Applications</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Zhen Liu, Hai Yan Zhang, Tu Pei Chen, Pan Liu, Sam Zhang, Wa Li Zhang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-11T10:36:13.432554-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12098</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12098</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12098</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Magnetron sputtering has been used to deposit Ni-rich nickel oxide thin films. Based on the switching of lateral current conduction in the nickel oxide thin film between two in-plane electrodes, a planar write-once-read-many-times memory device has been demonstrated. The switching from a low-conductance state (i.e., the OFF state) to a high-conductance state (i.e., the ON state) is induced by a writing voltage, and it is irreversible due to the formation of tilted conductive filaments that are hard to be dissolved by the Joule heating effect. For 80 devices under test, the writing voltage is in a narrow range of 2.0−3.5 V and the ON/OFF resistance ratio is larger than 10<sup>5</sup> at the reading voltage of 0.3 V. An excellent reading endurance (10<sup>6</sup> readings) for both ON and OFF states is demonstrated. The device is promising in low-power applications as it can operate at ultra-low voltages (e.g., the reading voltage can be below 100 mV).</p></div>
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Magnetron sputtering has been used to deposit Ni-rich nickel oxide thin films. Based on the switching of lateral current conduction in the nickel oxide thin film between two in-plane electrodes, a planar write-once-read-many-times memory device has been demonstrated. The switching from a low-conductance state (i.e., the OFF state) to a high-conductance state (i.e., the ON state) is induced by a writing voltage, and it is irreversible due to the formation of tilted conductive filaments that are hard to be dissolved by the Joule heating effect. For 80 devices under test, the writing voltage is in a narrow range of 2.0−3.5 V and the ON/OFF resistance ratio is larger than 105 at the reading voltage of 0.3 V. An excellent reading endurance (106 readings) for both ON and OFF states is demonstrated. The device is promising in low-power applications as it can operate at ultra-low voltages (e.g., the reading voltage can be below 100 mV).
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12041" xmlns="http://purl.org/rss/1.0/"><title>Effect of Heat Treatment Schedules and Glass Powder Particle Size on Glass Infiltration in Porous Alumina Preforms</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12041</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of Heat Treatment Schedules and Glass Powder Particle Size on Glass Infiltration in Porous Alumina Preforms</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Preeti Bajpai, Parag Bhargava</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-10T11:06:26.25125-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12041</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12041</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12041</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Glass infiltrated alumina is one of the popular materials for fabrication of dental prostheses. Achieving complete and uniform glass infiltration is important to achieve desired properties in dental prostheses. This study examined the role of various factors on glass infiltration in sintered porous alumina preforms (porosity ~ 27%). Observations on infiltration in porous alumina samples at a heating rate of 3°C/min at 1100°C for 2 h showed residual glass on the surfaces of the samples indicating incomplete infiltration. Rapid heating of the samples to the peak infiltration temperature by introducing the samples into a preheated furnace resulted in complete infiltration of glass into the samples in &lt;90 min. In addition to heating rate during infiltration, influence of soaking duration and the particle size of glass powder on glass infiltration were also examined.</p></div>
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Glass infiltrated alumina is one of the popular materials for fabrication of dental prostheses. Achieving complete and uniform glass infiltration is important to achieve desired properties in dental prostheses. This study examined the role of various factors on glass infiltration in sintered porous alumina preforms (porosity ~ 27%). Observations on infiltration in porous alumina samples at a heating rate of 3°C/min at 1100°C for 2 h showed residual glass on the surfaces of the samples indicating incomplete infiltration. Rapid heating of the samples to the peak infiltration temperature by introducing the samples into a preheated furnace resulted in complete infiltration of glass into the samples in &lt;90 min. In addition to heating rate during infiltration, influence of soaking duration and the particle size of glass powder on glass infiltration were also examined.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12084" xmlns="http://purl.org/rss/1.0/"><title>Dispersion and Rheology of Aqueous Zirconium Diboride Nanosuspensions</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12084</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Dispersion and Rheology of Aqueous Zirconium Diboride Nanosuspensions</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Rujie He, Ping Hu, Xinghong Zhang, Wenbo Han, Qin Wang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-09T13:52:16.144962-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12084</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12084</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12084</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The dispersion and rheology of aqueous ZrB<sub>2</sub> nanosuspensions were investigated by zeta potential measurements, particle size measurements, sedimentation tests, and rheology measurements, with poly (acrylic acid) (PAA) as dispersant. Results showed that the dispersion and rheology of nanosized ZrB<sub>2</sub> suspensions in aqueous media were dependent on pH value, PAA concentration, solid loading, and ball milling time. Concentrated (up to 30 vol% solid loading) and well-stabilized aqueous ZrB<sub>2</sub> nanosuspension with low viscosity (0.485 Pa s at 60/s) was prepared at pH 10, with 1.0 wt% PAA.</p></div>
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The dispersion and rheology of aqueous ZrB2 nanosuspensions were investigated by zeta potential measurements, particle size measurements, sedimentation tests, and rheology measurements, with poly (acrylic acid) (PAA) as dispersant. Results showed that the dispersion and rheology of nanosized ZrB2 suspensions in aqueous media were dependent on pH value, PAA concentration, solid loading, and ball milling time. Concentrated (up to 30 vol% solid loading) and well-stabilized aqueous ZrB2 nanosuspension with low viscosity (0.485 Pa s at 60/s) was prepared at pH 10, with 1.0 wt% PAA.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12057" xmlns="http://purl.org/rss/1.0/"><title>In Vitro Dissolution, Microstructural and Mechanical Characterizations of Microplasma-Sprayed Hydroxyapatite Coating</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12057</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">In Vitro Dissolution, Microstructural and Mechanical Characterizations of Microplasma-Sprayed Hydroxyapatite Coating</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Arjun Dey, Anoop K. Mukhopadhyay</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-09T13:52:09.205449-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12057</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12057</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12057</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Hydroxyapatite coating was developed with high degree of crystallinity on SS316L substrate by the microplasma spraying technique. Systematic <em>in vitro</em> study of the coating was conducted after the immersion into the simulated body fluid for 1–14 days. Inductively coupled plasma–atomic emission spectroscopy, X-ray diffraction, Fourier transformed infrared spectroscopy, and scanning electron microscopy were utilized for physicochemical and microstructural characterizations. Nanoindentation technique employed to evaluate the nanohardness and Young's modulus of the coating at a constant load of 100 mN. Further, the tribological characteristic was also examined by microscratch testing at a ramping normal load of 10–10.6 N.</p></div>
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Hydroxyapatite coating was developed with high degree of crystallinity on SS316L substrate by the microplasma spraying technique. Systematic in vitro study of the coating was conducted after the immersion into the simulated body fluid for 1–14 days. Inductively coupled plasma–atomic emission spectroscopy, X-ray diffraction, Fourier transformed infrared spectroscopy, and scanning electron microscopy were utilized for physicochemical and microstructural characterizations. Nanoindentation technique employed to evaluate the nanohardness and Young's modulus of the coating at a constant load of 100 mN. Further, the tribological characteristic was also examined by microscratch testing at a ramping normal load of 10–10.6 N.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12079" xmlns="http://purl.org/rss/1.0/"><title>Nanoscale Ceramics: Environmental, Health, and Safety (EHS) Implications</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12079</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Nanoscale Ceramics: Environmental, Health, and Safety (EHS) Implications</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sylvia M. Johnson, Lynnette D. Madsen, Stephen Freiman</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-08T11:03:24.237389-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12079</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12079</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12079</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Part of the symposium on Nanostructured Materials at the Fourth International Congress on Ceramics (ICC4) dealt with health aspects related to these materials. Major issues discussed included definitions and measurements of nanoparticles, best test protocols, collaboration and communication between, for example, materials scientists and biologists, and the plethora of information and regulations (that is sometimes even conflicting). Emerging opportunities were identified in terms of obtaining uniformity of nomenclature and testing standards, education and training of a new generation of multidisciplinary researchers, and understanding and then fully exploiting the positive aspects of nanomaterials, including improvements to human health.</p></div>
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Part of the symposium on Nanostructured Materials at the Fourth International Congress on Ceramics (ICC4) dealt with health aspects related to these materials. Major issues discussed included definitions and measurements of nanoparticles, best test protocols, collaboration and communication between, for example, materials scientists and biologists, and the plethora of information and regulations (that is sometimes even conflicting). Emerging opportunities were identified in terms of obtaining uniformity of nomenclature and testing standards, education and training of a new generation of multidisciplinary researchers, and understanding and then fully exploiting the positive aspects of nanomaterials, including improvements to human health.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12074" xmlns="http://purl.org/rss/1.0/"><title>Nanoceramics: Issues and Opportunities</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12074</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Nanoceramics: Issues and Opportunities</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Omer Biest</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-08T11:03:15.28244-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12074</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12074</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12074</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The goal of this study is to review developments in nanoceramics as discussed during presentations on the subject during the International Ceramic Congress (ICC4) held in Chicago on July 2012. As nanotechnology is such a broad subject affecting many industrial sectors, some presentations in other sessions were included as well. The study has been organized according to the dimensions of the nanoscale material starting with nanoscale entities or particulates followed by nanothin films and finally bulk nanoceramics where the nanoscale character lies in the structure. Developments on hybrid nanocomposites containing at least one ceramic compound were often included in the presentations and are discussed in a separate section. The promise of nanotechnology is also to discover materials with totally new properties or combinations of properties. One such example presented in depth at the conference is presented. The study concludes with a section on issues and opportunities. In general, it can be said that the very large investments that were made more than a decade ago into nanotechnology start to pay off dividends. Products are appearing on the market and can have a substantial impact there. Other commercial applications are on the horizon. Because of the wide scope of the technology, there are still plenty of opportunities for research and development. A particular issue that was mentioned by a number of speakers is that of upscaling, which can be understood literally as interfacing the nanostructure with the micro-, meso-, and macroworld. However, often one means the implementation on the factory floor of processes that have been developed within the laboratory.</p></div>
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The goal of this study is to review developments in nanoceramics as discussed during presentations on the subject during the International Ceramic Congress (ICC4) held in Chicago on July 2012. As nanotechnology is such a broad subject affecting many industrial sectors, some presentations in other sessions were included as well. The study has been organized according to the dimensions of the nanoscale material starting with nanoscale entities or particulates followed by nanothin films and finally bulk nanoceramics where the nanoscale character lies in the structure. Developments on hybrid nanocomposites containing at least one ceramic compound were often included in the presentations and are discussed in a separate section. The promise of nanotechnology is also to discover materials with totally new properties or combinations of properties. One such example presented in depth at the conference is presented. The study concludes with a section on issues and opportunities. In general, it can be said that the very large investments that were made more than a decade ago into nanotechnology start to pay off dividends. Products are appearing on the market and can have a substantial impact there. Other commercial applications are on the horizon. Because of the wide scope of the technology, there are still plenty of opportunities for research and development. A particular issue that was mentioned by a number of speakers is that of upscaling, which can be understood literally as interfacing the nanostructure with the micro-, meso-, and macroworld. However, often one means the implementation on the factory floor of processes that have been developed within the laboratory.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12082" xmlns="http://purl.org/rss/1.0/"><title>Effects of A-Site Sm Substitution and Textured Structure on Electric Properties of CaBi2Nb2O9-Based High-Curie-Temperature Ceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12082</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effects of A-Site Sm Substitution and Textured Structure on Electric Properties of CaBi2Nb2O9-Based High-Curie-Temperature Ceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Huanbei Chen, Xiangxin Guo, Zhonghui Cui, Jiwei Zhai</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-08T11:03:05.758505-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12082</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12082</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12082</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>CaBi<sub>2</sub>Nb<sub>2</sub>O<sub>9</sub> ceramic is a promising candidate for high-temperature piezoelectric applications due to its high Curie temperature. However, extremely low piezoelectric properties hinder its application. A combination of Sm<sup>3+</sup> donor doping and texturing was applied to address this problem. Piezoelectric coefficient, <em>T</em><sub>c</sub>, and resistivity of textured Ca<sub>0.95</sub>Sm<sub>0.05</sub>Bi<sub>2</sub>Nb<sub>2</sub>O<sub>9</sub> ceramics (<em>d</em><sub>33</sub><em> </em>=<em> </em>23pC/N, <em>T</em><sub>c</sub> = 941°C, <em>ρ </em>= 4.1 × 10<sup>5</sup>Ω cm at 600°C) were obviously higher than those of pure random CaBi<sub>2</sub>Nb<sub>2</sub>O<sub>9</sub> ceramics (<em>d</em><sub>33</sub><em> </em>=<em> </em>6, <em>T</em><sub>c</sub> = 930°C, <em>ρ</em>=0.6 × 10<sup>5</sup>Ω cm at 600°C). Furthermore, it had excellent resistance to depolarization property, with <em>k</em><sub>p</sub> of about 5.9% until 600°C.</p></div>
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CaBi2Nb2O9 ceramic is a promising candidate for high-temperature piezoelectric applications due to its high Curie temperature. However, extremely low piezoelectric properties hinder its application. A combination of Sm3+ donor doping and texturing was applied to address this problem. Piezoelectric coefficient, Tc, and resistivity of textured Ca0.95Sm0.05Bi2Nb2O9 ceramics (d33 = 23pC/N, Tc = 941°C, ρ = 4.1 × 105Ω cm at 600°C) were obviously higher than those of pure random CaBi2Nb2O9 ceramics (d33 = 6, Tc = 930°C, ρ=0.6 × 105Ω cm at 600°C). Furthermore, it had excellent resistance to depolarization property, with kp of about 5.9% until 600°C.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12001" xmlns="http://purl.org/rss/1.0/"><title>A Simple Way to Prepare C/SiC Spring</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12001</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A Simple Way to Prepare C/SiC Spring</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Si'an Chen, Yudi Zhang, Changrui Zhang, Xin Xiong, Guangde Li, Haifeng Hu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-08T11:02:49.747114-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12001</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12001</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12001</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A new method to form helical C/SiC spring is proposed. Using paraffin mold as a sacrificial core, unidirectional carbon fiber bundles (infiltrated with resin) are wrapped around the mold to form helical spring, and after resin curing, the mold is removed, leaving a preform of C/SiC spring. Following densification is finished with precursor infiltration and pyrolysis (PIP) process. The spring constant of C/SiC spring reaches 7.88 N/mm and could be regulated by varying composite density and carbon fiber content. The spring properties could be improved by twisting the carbon fibers at 35–50 twist/m. The restoration ratio reaches 100%, but energy dissipation happens during unloading process. After oxidation in air at 1200°C for 10 min, the spring has an 82.4% spring constant remaining ratio.</p></div>
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A new method to form helical C/SiC spring is proposed. Using paraffin mold as a sacrificial core, unidirectional carbon fiber bundles (infiltrated with resin) are wrapped around the mold to form helical spring, and after resin curing, the mold is removed, leaving a preform of C/SiC spring. Following densification is finished with precursor infiltration and pyrolysis (PIP) process. The spring constant of C/SiC spring reaches 7.88 N/mm and could be regulated by varying composite density and carbon fiber content. The spring properties could be improved by twisting the carbon fibers at 35–50 twist/m. The restoration ratio reaches 100%, but energy dissipation happens during unloading process. After oxidation in air at 1200°C for 10 min, the spring has an 82.4% spring constant remaining ratio.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12081" xmlns="http://purl.org/rss/1.0/"><title>Flexible Hydrophobic and Lipophilic Aluminum-Doped Silicon Carbide Fibrous Mats Synthesized by Electrospinning Polyaluminocarbosilane</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12081</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Flexible Hydrophobic and Lipophilic Aluminum-Doped Silicon Carbide Fibrous Mats Synthesized by Electrospinning Polyaluminocarbosilane</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yuxi Yu, Yong Chen, Linan An</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-08T10:58:03.136812-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12081</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12081</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12081</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Flexible aluminum-doped silicon carbide (SiC(Al)) fibrous mats were synthesized by combining electrospinning and polymer-derived ceramic techniques. The mats consist of three-dimensional network structure with randomly distributed fibers of approximately 1.5 μm diameter. The obtained mats exhibited simultaneous fairly good hydrophobic and lipophilic behavior without the need of any posttreatment. Given the intrinsic oxidation/corrosion resistance of Al-doped SiC, the ceramic mats obtained here could be very promising for applications in harsh environments.</p></div>
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Flexible aluminum-doped silicon carbide (SiC(Al)) fibrous mats were synthesized by combining electrospinning and polymer-derived ceramic techniques. The mats consist of three-dimensional network structure with randomly distributed fibers of approximately 1.5 μm diameter. The obtained mats exhibited simultaneous fairly good hydrophobic and lipophilic behavior without the need of any posttreatment. Given the intrinsic oxidation/corrosion resistance of Al-doped SiC, the ceramic mats obtained here could be very promising for applications in harsh environments.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12058" xmlns="http://purl.org/rss/1.0/"><title>Influence of Oxygen Substoichiometry on the Dielectric Properties of BaTiO3-δ Nanoceramics Obtained by Spark Plasma Sintering</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12058</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Influence of Oxygen Substoichiometry on the Dielectric Properties of BaTiO3-δ Nanoceramics Obtained by Spark Plasma Sintering</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Christophe Voisin, Sophie Guillemet-Fritsch, Pascal Dufour, Christophe Tenailleau, Hyuksu Han, Juan C. Nino</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-08T10:57:47.860623-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12058</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12058</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12058</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Oxygen-deficient BaTiO<sub>3-δ</sub> nanoceramics were prepared by spark plasma sintering. Partially reduced raw nanopowders led to unusual dielectric properties. A short postsintering treatment was performed to reach a high ε<sub>r</sub>/tan δ, which makes them attractive for industrial applications such as low-frequency capacitors. Surprisingly, our ceramics also remained black even after annealing for 5 days at 850°C in air, indicating the presence of barriers against oxygen diffusion. This exceptional behavior in pure barium titanate was consistent with a core–shell structure made of semiconductive grains and insulating grain boundaries, due to the presence of Ti<sup>3+</sup>/Ti<sup>4+</sup> and oxygen vacancies.</p></div>
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Oxygen-deficient BaTiO3-δ nanoceramics were prepared by spark plasma sintering. Partially reduced raw nanopowders led to unusual dielectric properties. A short postsintering treatment was performed to reach a high εr/tan δ, which makes them attractive for industrial applications such as low-frequency capacitors. Surprisingly, our ceramics also remained black even after annealing for 5 days at 850°C in air, indicating the presence of barriers against oxygen diffusion. This exceptional behavior in pure barium titanate was consistent with a core–shell structure made of semiconductive grains and insulating grain boundaries, due to the presence of Ti3+/Ti4+ and oxygen vacancies.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12073" xmlns="http://purl.org/rss/1.0/"><title>Influence of R3+ Ion Sizes on the Transport Properties of RBaCo2O5+δ Ceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12073</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Influence of R3+ Ion Sizes on the Transport Properties of RBaCo2O5+δ Ceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Zhen Qin, Hongzhang Song, Feng Gao, Jianfeng Jia, Delin Yang, Xing Hu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-08T10:57:30.795432-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12073</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12073</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12073</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The resistivity, Seebeck coefficients, and power factors of as-prepared RBaCo<sub>2</sub>O<sub>5+δ</sub> (R112) ceramics with variable R<sup>3+</sup> ion sizes were investigated systemically. The resistivity of Pr112 and Nd112 exhibits semimetal behavior, which is different with other R112 who have a semiconductor-semimetal transition. At room temperature, Dy112 has the biggest Seebeck coefficient. While at higher temperature, Y112 has best thermoelectric power. In addition, the affects of normalizing temperature on the transport properties of Eu112 ceramic were investigated. Its power factor above room temperature is improved by normalizing, and an optimum normalizing temperature exists at 400°C.</p></div>
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The resistivity, Seebeck coefficients, and power factors of as-prepared RBaCo2O5+δ (R112) ceramics with variable R3+ ion sizes were investigated systemically. The resistivity of Pr112 and Nd112 exhibits semimetal behavior, which is different with other R112 who have a semiconductor-semimetal transition. At room temperature, Dy112 has the biggest Seebeck coefficient. While at higher temperature, Y112 has best thermoelectric power. In addition, the affects of normalizing temperature on the transport properties of Eu112 ceramic were investigated. Its power factor above room temperature is improved by normalizing, and an optimum normalizing temperature exists at 400°C.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12018" xmlns="http://purl.org/rss/1.0/"><title>A Comparison on Physical, Structural, and Photocatalytical Properties of TiO2 Nanopowders Produced Using Sol-Gel and Flame Spray Pyrolysis</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12018</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A Comparison on Physical, Structural, and Photocatalytical Properties of TiO2 Nanopowders Produced Using Sol-Gel and Flame Spray Pyrolysis</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mustafa Erol, Orkut Sancakoglu, Metin Yurddaskal, Serdar Yildirim, Erdal Çelik</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-03T13:25:30.834036-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12018</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12018</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12018</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>In this study, nanoscale photocatalyst TiO<sub>2</sub> powders were synthesized via sol-gel and flame spray pyrolysis (FSP). Phase structures and ratios were analyzed by X-ray diffractometer (XRD). Size, specific surface area, and morphologies were determined using particle size analyzer, Brunauer-Emmett-Teller theory, and scanning electron microscope, respectively. Anatase phase with some rutile together was obtained in XRD analysis. The degradation rates of aqueous methylene blue (MB) by TiO<sub>2</sub> nanopowders were calculated using UV–vis spectrophotometer. It was found that MB decomposition was successfully achieved with significantly high efficiencies for both sol-gel and FSP-derived powders with small differences.</p></div>
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In this study, nanoscale photocatalyst TiO2 powders were synthesized via sol-gel and flame spray pyrolysis (FSP). Phase structures and ratios were analyzed by X-ray diffractometer (XRD). Size, specific surface area, and morphologies were determined using particle size analyzer, Brunauer-Emmett-Teller theory, and scanning electron microscope, respectively. Anatase phase with some rutile together was obtained in XRD analysis. The degradation rates of aqueous methylene blue (MB) by TiO2 nanopowders were calculated using UV–vis spectrophotometer. It was found that MB decomposition was successfully achieved with significantly high efficiencies for both sol-gel and FSP-derived powders with small differences.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02845.x" xmlns="http://purl.org/rss/1.0/"><title>Effects of Particle Size on Soft Lithography Process, the Green and Sintered Micro Alumina Parts</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02845.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effects of Particle Size on Soft Lithography Process, the Green and Sintered Micro Alumina Parts</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hany Hassanin, Kyle Jiang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-03T13:25:26.046364-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02845.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02845.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02845.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Alumina micro parts were fabricated using powders in particle sizes of 1 μm, 2.0 μm, and 12.0 μm. The effects of particle size on soft lithography process, green bodies, and sintered characteristics were investigated, including process parameters affecting homogeneous and smooth surface. The effects of particle size were analyzed through suspensions, green, and sintered properties. It was found that the stability of suspensions, sintered density, Vickers micro hardness, surface roughness and edges resolution are significantly improved with the decrease in particle size. On the other hand, suspension viscosity, green density and shrinkage are degraded with the use of finer particles.</p></div>
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Alumina micro parts were fabricated using powders in particle sizes of 1 μm, 2.0 μm, and 12.0 μm. The effects of particle size on soft lithography process, green bodies, and sintered characteristics were investigated, including process parameters affecting homogeneous and smooth surface. The effects of particle size were analyzed through suspensions, green, and sintered properties. It was found that the stability of suspensions, sintered density, Vickers micro hardness, surface roughness and edges resolution are significantly improved with the decrease in particle size. On the other hand, suspension viscosity, green density and shrinkage are degraded with the use of finer particles.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02836.x" xmlns="http://purl.org/rss/1.0/"><title>Effect of Heat on Hollow Multiphase Ceramic Microspheres Prepared by Self-Reactive Quenching Technology</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02836.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of Heat on Hollow Multiphase Ceramic Microspheres Prepared by Self-Reactive Quenching Technology</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Lou Hongfei, Wang Jianjiang, Huo Xingjian, Cai Xudong</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-03T13:25:22.68358-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02836.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02836.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02836.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The self-reactive quenching technology, which combines flame thermal spraying technology, self-propagating high-temperature synthesis (SHS), and rapid solidification, is a new method for preparation of hollow microspheres. Based on this, the effect of heat released by different exothermic systems on preparation of hollow ceramic microspheres was studied. The results show that for low-exothermic system <span class="fixed-roman">Si</span>-Sucrose-<span class="fixed-roman">NH</span><sub>4</sub><span class="fixed-roman">Cl</span>, the self-propagating reactions cannot occur, and the quenching products are <span class="fixed-roman">Si</span> microspheres with porous structure. For the moderate exothermic system <span class="fixed-roman">Al</span>–<span class="fixed-roman">SiO</span><sub>2</sub>-Sucrose, the quenching products consist of some grains, which are hollow spherical or nearly spherical particles and irregular powders. Formation of <span class="fixed-roman">Al</span><sub>2</sub><span class="fixed-roman">O</span><sub>3</sub>–<span class="fixed-roman">Si</span> indicates possible occurrence of SHS reactions. Meanwhile, for high-exothermic system <span class="fixed-roman">Al</span>–<span class="fixed-roman">Cr</span><sub>2</sub><span class="fixed-roman">O</span><sub>3</sub>-Sucrose-<span class="fixed-roman">Si</span>-Epoxy Resin, the quenching products consist of internal hollow spherical grains and irregular-shaped porous particles; the phase composition mainly contains <span class="fixed-roman">Al</span><sub>2</sub><span class="fixed-roman">O</span><sub>3</sub>, <span class="fixed-roman">Cr</span><sub>3</sub><span class="fixed-roman">C</span><sub>2</sub>, <span class="fixed-roman">Cr</span><sub>7</sub><span class="fixed-roman">C</span><sub>3</sub>, <span class="fixed-roman">Cr</span><sub>3</sub><span class="fixed-roman">Si</span>, and mullite, showing completeness of SHS reactions. The higher the adiabatic combustion temperature of the system is, the more heat it releases is higher, and the ceramic droplets form easilier.</p></div>
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The self-reactive quenching technology, which combines flame thermal spraying technology, self-propagating high-temperature synthesis (SHS), and rapid solidification, is a new method for preparation of hollow microspheres. Based on this, the effect of heat released by different exothermic systems on preparation of hollow ceramic microspheres was studied. The results show that for low-exothermic system Si-Sucrose-NH4Cl, the self-propagating reactions cannot occur, and the quenching products are Si microspheres with porous structure. For the moderate exothermic system Al–SiO2-Sucrose, the quenching products consist of some grains, which are hollow spherical or nearly spherical particles and irregular powders. Formation of Al2O3–Si indicates possible occurrence of SHS reactions. Meanwhile, for high-exothermic system Al–Cr2O3-Sucrose-Si-Epoxy Resin, the quenching products consist of internal hollow spherical grains and irregular-shaped porous particles; the phase composition mainly contains Al2O3, Cr3C2, Cr7C3, Cr3Si, and mullite, showing completeness of SHS reactions. The higher the adiabatic combustion temperature of the system is, the more heat it releases is higher, and the ceramic droplets form easilier.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12019" xmlns="http://purl.org/rss/1.0/"><title>Clinical Satisfaction and Quality of Ceramic Fixed Dentures</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12019</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Clinical Satisfaction and Quality of Ceramic Fixed Dentures</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Marcelo Coelho Goiato, Aldiéris Alves Pesqueira, Douglas Roberto Monteiro, Daniel Augusto Faria Almeida, Daniela Micheline Santos</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-03T11:49:29.160305-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12019</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12019</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12019</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>It is known that several factors can affect the clinical success and durability of fixed partial dentures. Therefore, the aim of the present study was to present a literature review about the longevity, clinical success, and quality, as well as, patients' and dental surgeons' satisfaction of ceramic fixed dentures. High rate of patients' satisfaction has been observed in relation to the esthetic of ceramic crowns. In addition, the literature has shown that dental ceramics can be used in several clinical situations with high success rate and longevity. Despite of failures and complications of ceramic restorations, nowadays, with the improvement of mechanical properties of such materials, ceramic crowns present a favorable prognosis and can be used in several clinical situations with high success rate, clinical quality, and great patients' satisfaction.</p></div>
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It is known that several factors can affect the clinical success and durability of fixed partial dentures. Therefore, the aim of the present study was to present a literature review about the longevity, clinical success, and quality, as well as, patients' and dental surgeons' satisfaction of ceramic fixed dentures. High rate of patients' satisfaction has been observed in relation to the esthetic of ceramic crowns. In addition, the literature has shown that dental ceramics can be used in several clinical situations with high success rate and longevity. Despite of failures and complications of ceramic restorations, nowadays, with the improvement of mechanical properties of such materials, ceramic crowns present a favorable prognosis and can be used in several clinical situations with high success rate, clinical quality, and great patients' satisfaction.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12017" xmlns="http://purl.org/rss/1.0/"><title>Preparation of Ag-AZO Nanocomposite Powder Compact for RF Magnetron Sputtering Target Application</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12017</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Preparation of Ag-AZO Nanocomposite Powder Compact for RF Magnetron Sputtering Target Application</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Joseph Lik Hang Chau, Yu-Hsien Chou, Shun-Huei Wang,, Chih-Chao Yang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-03T11:49:25.385735-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12017</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12017</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12017</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Octylamine-coated silver nanoparticles with an average size of 10 nm were synthesized and added to the AZO powder as fillers to increase the density of the sintered target. The resulting Ag–AZO nanocomposite powder was formed into compacts by a uniaxial pressing process. It was found that the addition of octylamine- coated silver nanoparticles can increase the density of AZO powder compacts by ~ 4% after sintering. The optimum content of silver addition is about 0.13 wt%. It is suggested that the melted silver fills the void space between agglomerate pores and enhances the interconnection between nanocrystalline AZO powders. The films deposited using the here-synthesized Ag–AZO target showed lower resistivity and high carrier concentration compared with the one using AZO target.</p></div>
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Octylamine-coated silver nanoparticles with an average size of 10 nm were synthesized and added to the AZO powder as fillers to increase the density of the sintered target. The resulting Ag–AZO nanocomposite powder was formed into compacts by a uniaxial pressing process. It was found that the addition of octylamine- coated silver nanoparticles can increase the density of AZO powder compacts by ~ 4% after sintering. The optimum content of silver addition is about 0.13 wt%. It is suggested that the melted silver fills the void space between agglomerate pores and enhances the interconnection between nanocrystalline AZO powders. The films deposited using the here-synthesized Ag–AZO target showed lower resistivity and high carrier concentration compared with the one using AZO target.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12056" xmlns="http://purl.org/rss/1.0/"><title>Multilayer Ultrabroadband Piezocomposite Transducer: Fabrication and Characterization</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12056</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Multilayer Ultrabroadband Piezocomposite Transducer: Fabrication and Characterization</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Erman Uzgur</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-26T07:56:54.61215-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12056</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12056</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12056</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The broad bandwidth is essential for the ultrasonic transducers because of two main reasons: Firstly, the image axial resolution can be improved by broad bandwidth, and secondly, the ultrasound scanning flexibility can be improved by operating the transducer over a wide range of frequencies. Particularly, nonlinear applications such as biomedical imaging that requires transmitting and receiving in different frequencies can utilize broadband characteristics of transducer efficiently. In this study, a dual-layer piezocomposite transducer was designed by combining two 1–3 piezocomposite transducers with various thicknesses to couple their resonance frequencies and to increase the bandwidth. PZFlex code was used to determine the most promising layer thicknesses for elements of multilayer structure coupling. Finite element analysis showed that the best thickness combination is 1.2 mm and 2 mm. After fabricating multilayer transducers by traditional dice and fill method, their characteristics were examined under water by Labview automated measurement system. Relative sound pressure produced by the transducer was obtained, and their bandwidth was examined at −3 and −6 dB. By varying the individual active layer thicknesses, acoustic impedance of the backing layer and coupling material the best promising broadband transducer design was reported. In addition, ringing characteristics of the transducers were identified by performing the pulse–echo testing. Multilayer transducer with 1.2 mm and 2 mm layer thicknesses and 6 MRayls backing layer gave the best performance in terms of bandwidth and ringing characteristics.</p></div>
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The broad bandwidth is essential for the ultrasonic transducers because of two main reasons: Firstly, the image axial resolution can be improved by broad bandwidth, and secondly, the ultrasound scanning flexibility can be improved by operating the transducer over a wide range of frequencies. Particularly, nonlinear applications such as biomedical imaging that requires transmitting and receiving in different frequencies can utilize broadband characteristics of transducer efficiently. In this study, a dual-layer piezocomposite transducer was designed by combining two 1–3 piezocomposite transducers with various thicknesses to couple their resonance frequencies and to increase the bandwidth. PZFlex code was used to determine the most promising layer thicknesses for elements of multilayer structure coupling. Finite element analysis showed that the best thickness combination is 1.2 mm and 2 mm. After fabricating multilayer transducers by traditional dice and fill method, their characteristics were examined under water by Labview automated measurement system. Relative sound pressure produced by the transducer was obtained, and their bandwidth was examined at −3 and −6 dB. By varying the individual active layer thicknesses, acoustic impedance of the backing layer and coupling material the best promising broadband transducer design was reported. In addition, ringing characteristics of the transducers were identified by performing the pulse–echo testing. Multilayer transducer with 1.2 mm and 2 mm layer thicknesses and 6 MRayls backing layer gave the best performance in terms of bandwidth and ringing characteristics.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12055" xmlns="http://purl.org/rss/1.0/"><title>Measurement of the Stress in Oxide Scales Developed Upon Oxidation of a Pt-Based Alloy in Air at 1250°C</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12055</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Measurement of the Stress in Oxide Scales Developed Upon Oxidation of a Pt-Based Alloy in Air at 1250°C</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jamiu Kolawole Odusote, Lesley Alison Cornish, Lesley Heath Chown, Rudolph Marthinus Erasmus</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-26T07:56:49.129176-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12055</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12055</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12055</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The nature and magnitude of stress in the scales formed on Pt-11Al-3Cr-2Ru (at.%) alloy oxidized in air at 1250°C, for up to 500 h, were determined. This is to establish their long-term viability during high-temperature applications. Residual stress in the scales was measured using luminescence piezospectroscopy and found to be compressive. It decreased gradually with increased oxidation time, before reaching a constant value. The compressive stress was also found to be lower than those of other Ni- and Fe-based superalloys. Thus, the current alloy has a promising potential for high-temperature applications.</p></div>
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The nature and magnitude of stress in the scales formed on Pt-11Al-3Cr-2Ru (at.%) alloy oxidized in air at 1250°C, for up to 500 h, were determined. This is to establish their long-term viability during high-temperature applications. Residual stress in the scales was measured using luminescence piezospectroscopy and found to be compressive. It decreased gradually with increased oxidation time, before reaching a constant value. The compressive stress was also found to be lower than those of other Ni- and Fe-based superalloys. Thus, the current alloy has a promising potential for high-temperature applications.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12049" xmlns="http://purl.org/rss/1.0/"><title>Formation of CuAlO2 at the Cu/Al2O3 Interface and its Influence on Interface Strength and Thermal Conductivity</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12049</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Formation of CuAlO2 at the Cu/Al2O3 Interface and its Influence on Interface Strength and Thermal Conductivity</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Shao-Kuan Lee, Wei-Hsing Tuan</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-25T10:45:43.531329-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12049</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12049</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12049</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The criteria for the formation of a CuAlO<sub>2</sub> reaction phase at the Cu/Al<sub>2</sub>O<sub>3</sub> interface are explored. Oxygen solutes up to 2 wt% were introduced into the copper first. The bonding was carried out at 1075°C. The reaction phase was observed only when the oxygen solute in copper before bonding was higher than 1.3 wt%. The CuAlO<sub>2</sub> phase is polycrystalline and covers only part of the interface. The CuAlO<sub>2</sub> grains interact with the crack, which improves the interface strength. As CuAlO<sub>2</sub> is not continuous at the interface, the thermal conductivity of the Al<sub>2</sub>O<sub>3</sub>/Cu/Al<sub>2</sub>O<sub>3</sub> laminate is affected little.</p></div>
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The criteria for the formation of a CuAlO2 reaction phase at the Cu/Al2O3 interface are explored. Oxygen solutes up to 2 wt% were introduced into the copper first. The bonding was carried out at 1075°C. The reaction phase was observed only when the oxygen solute in copper before bonding was higher than 1.3 wt%. The CuAlO2 phase is polycrystalline and covers only part of the interface. The CuAlO2 grains interact with the crack, which improves the interface strength. As CuAlO2 is not continuous at the interface, the thermal conductivity of the Al2O3/Cu/Al2O3 laminate is affected little.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12053" xmlns="http://purl.org/rss/1.0/"><title>The Effect of the Two-Step Sintering Process on Consolidation of Fluoridated Hydroxyapatite and its Mechanical Properties and Bioactivity</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12053</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">The Effect of the Two-Step Sintering Process on Consolidation of Fluoridated Hydroxyapatite and its Mechanical Properties and Bioactivity</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mohammadhossein Esnaashary,, Mohammadhossein Fathi, Mahdi Ahmadian</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-25T10:45:33.900293-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12053</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12053</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12053</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The aim of this work was to evaluate the effect of the two-step sintering process on consolidation of fluoridated hydroxyapatite (FHA). In addition, the effect of fluorine content on sinterability, mechanical properties, and bioactivity of FHA bulks was studied. Nanostructured FHA bulks were obtained under the conditions of 1000 and 900°C for the initial and secondary temperatures, respectively, without any structural decomposition. In addition, by increasing the fluorine content, the sinterability of FHA bulks was decreased and the hardness of FHA bulks was improved. Moreover, FHA bulks showed acceptable bioactivity.</p></div>
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The aim of this work was to evaluate the effect of the two-step sintering process on consolidation of fluoridated hydroxyapatite (FHA). In addition, the effect of fluorine content on sinterability, mechanical properties, and bioactivity of FHA bulks was studied. Nanostructured FHA bulks were obtained under the conditions of 1000 and 900°C for the initial and secondary temperatures, respectively, without any structural decomposition. In addition, by increasing the fluorine content, the sinterability of FHA bulks was decreased and the hardness of FHA bulks was improved. Moreover, FHA bulks showed acceptable bioactivity.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12050" xmlns="http://purl.org/rss/1.0/"><title>Synthesis of a Violet Sr–Al–O:Eu2+ Phosphor Particle Using Elemental Al Diffusion</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12050</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Synthesis of a Violet Sr–Al–O:Eu2+ Phosphor Particle Using Elemental Al Diffusion</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Keiji Komatsu, Shinya Tsuchida, Hayato Maruyama, Shigeo Ohshio, Hiroki Akasaka, Hidetoshi Saitoh, Atsushi Nakamura</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-25T10:44:40.117199-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12050</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12050</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12050</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A violet divalent europium-doped strontium aluminate (Sr–Al–O:Eu<sup>2+</sup>) phosphor particle was synthesized from a metal-ethylenediaminetetraacetic acid (EDTA) solution of Sr, Al, Eu, and particulate alumina via spray drying and sintering in a reducing atmosphere. The emission properties, crystal structures, cross-sectional emissions, and elemental distributions of the obtained Sr–Al–O:Eu<sup>2+</sup> phosphor particles were investigated. The product was determined to be secondary SrAl<sub>12</sub>O<sub>19</sub>:Eu<sup>2+</sup> particles with an average diameter of 20 μm. The violet SrAl<sub>12</sub>O<sub>19</sub>:Eu<sup>2+</sup> emission phase was found in a 1-μm-thick coating of the particles where elemental Al diffusion occurred. These particles are anticipated to find commercial applications such as paints.</p></div>
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A violet divalent europium-doped strontium aluminate (Sr–Al–O:Eu2+) phosphor particle was synthesized from a metal-ethylenediaminetetraacetic acid (EDTA) solution of Sr, Al, Eu, and particulate alumina via spray drying and sintering in a reducing atmosphere. The emission properties, crystal structures, cross-sectional emissions, and elemental distributions of the obtained Sr–Al–O:Eu2+ phosphor particles were investigated. The product was determined to be secondary SrAl12O19:Eu2+ particles with an average diameter of 20 μm. The violet SrAl12O19:Eu2+ emission phase was found in a 1-μm-thick coating of the particles where elemental Al diffusion occurred. These particles are anticipated to find commercial applications such as paints.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12011" xmlns="http://purl.org/rss/1.0/"><title>Structure and Microwave Dielectric Characteristics of Solid Solutions in SrNdAlO4-Sr2TiO4 System</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12011</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Structure and Microwave Dielectric Characteristics of Solid Solutions in SrNdAlO4-Sr2TiO4 System</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Chao Zhang, Lei Yi, Lei Li, Xiang Ming Chen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T12:26:00.424325-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12011</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12011</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12011</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Dense ceramics in SrNdAlO<sub>4</sub>-Sr<sub>2</sub>TiO<sub>4</sub> system were synthesized by a solid-state reaction method, and their microstructures and microwave dielectric characteristics were investigated. The K<sub>2</sub>NiF<sub>4</sub>-type solid solutions with general formula Sr<sub>1+</sub><sub><em>x</em></sub>Nd<sub>1-</sub><sub><em>x</em></sub>Al<sub>1-</sub><sub><em>x</em></sub>Ti<sub><em>x</em></sub>O<sub>4</sub> were obtained in the entire composition range (0.05 ≤ <em>x </em>≤<em> </em>0.9). With increasing <em>x</em>, the dielectric constant ε<sub><em>r</em></sub> increased from 19.2 to 25, and the temperature coefficient of resonant frequency τ<sub><em>f</em></sub> was adjusted from −16.7 to 24.6 ppm/°C. The significantly improved <em>Qf</em> value was achieved in the present ceramics with increasing <em>x</em>, and it reached a maximum at <em>x </em>=<em> </em>0.6. The best combination of microwave dielectric characteristics was achieved at <em>x </em>=<em> </em>0.6 (ε<sub><em>r</em> </sub>= 23.6, <em>Qf </em>= 86,300 GHz, τ<sub><em>f </em></sub>= 10.9 ppm/<sup>o</sup>C). The reduced interlayer polarization with Sr/Ti cosubstitution in SrNdAlO<sub>4</sub> contributed to the improved <em>Qf</em>, while the decreased tolerance factor and increased inner stress brought the negative effects.</p></div>
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Dense ceramics in SrNdAlO4-Sr2TiO4 system were synthesized by a solid-state reaction method, and their microstructures and microwave dielectric characteristics were investigated. The K2NiF4-type solid solutions with general formula Sr1+xNd1-xAl1-xTixO4 were obtained in the entire composition range (0.05 ≤ x ≤ 0.9). With increasing x, the dielectric constant εr increased from 19.2 to 25, and the temperature coefficient of resonant frequency τf was adjusted from −16.7 to 24.6 ppm/°C. The significantly improved Qf value was achieved in the present ceramics with increasing x, and it reached a maximum at x = 0.6. The best combination of microwave dielectric characteristics was achieved at x = 0.6 (εr = 23.6, Qf = 86,300 GHz, τf = 10.9 ppm/oC). The reduced interlayer polarization with Sr/Ti cosubstitution in SrNdAlO4 contributed to the improved Qf, while the decreased tolerance factor and increased inner stress brought the negative effects.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12010" xmlns="http://purl.org/rss/1.0/"><title>Development of New Cordierite-Based Refractory Coatings for Casting Applications</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12010</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Development of New Cordierite-Based Refractory Coatings for Casting Applications</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Aurel Prstić, Zagorka Aćimović-Pavlović, Anja Terzić, Ljubica Pavlović, Snežana Grujić</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T12:25:39.738738-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12010</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12010</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12010</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>In this study, new refractory coatings based on synthesized cordierite for the casting applications were developed. The investigation included starting raw materials characterization, synthesis of the cordierite, design of the refractory coating as final product, and its application testing. The obtained results pointed out that coating suspension sediment stability was crucial quality parameter. Design and optimization of the coatings composition, with controlled rheological properties included, were achieved by application of different coating components, namely different suspension agents and by alteration of the coating production procedure. Cordierite, used as filler, was obtained by means of synthesis in the solid-state reaction on the basis of talc, kaolin, and alumina. The investigation showed that the application of these particular types of water/alcohol-based coatings has positive influence on surface quality and structural and mechanical properties of the castings of aluminum alloys obtained by casting into sand molds by means of evaporable models method, that is, evaporate pattern casting process.</p></div>
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In this study, new refractory coatings based on synthesized cordierite for the casting applications were developed. The investigation included starting raw materials characterization, synthesis of the cordierite, design of the refractory coating as final product, and its application testing. The obtained results pointed out that coating suspension sediment stability was crucial quality parameter. Design and optimization of the coatings composition, with controlled rheological properties included, were achieved by application of different coating components, namely different suspension agents and by alteration of the coating production procedure. Cordierite, used as filler, was obtained by means of synthesis in the solid-state reaction on the basis of talc, kaolin, and alumina. The investigation showed that the application of these particular types of water/alcohol-based coatings has positive influence on surface quality and structural and mechanical properties of the castings of aluminum alloys obtained by casting into sand molds by means of evaporable models method, that is, evaporate pattern casting process.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12009" xmlns="http://purl.org/rss/1.0/"><title>Enhancement of Dielectric Characteristics of Polyvinyl Alcohol (PVA) Interfacial Layer in Au/PVA/n-Si Structures by Bi2O3 Disperse</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12009</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Enhancement of Dielectric Characteristics of Polyvinyl Alcohol (PVA) Interfacial Layer in Au/PVA/n-Si Structures by Bi2O3 Disperse</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Muharrem Gökçen, Tuncay Tunç</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T12:25:23.237935-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12009</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12009</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12009</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Dielectric characteristics such as dielectric constant (ε′), dielectric loss (ε″), dielectric loss tangent (tanδ) and real and imaginary parts of electrical modulus (<em>Μ</em>′ and <em>Μ</em>″), and <em>ac</em> electrical conductivity (<em>σ</em><sub><em>ac</em></sub>) of Au/ Polyvinyl Alcohol (PVA) (Bi<sub>2</sub>O<sub>3</sub>-dispersed)/n-Si structures have been investigated by using admittance measurements. Results show that the ε′ values of Au/PVA/n-Si with Bi<sub>2</sub>O<sub>3</sub>-dispersed PVA interfacial layer are very higher compared with those with pure and other dopant/mixture's of PVA. Thus, PVA is made very compatible for device applications with the enhanced dielectric properties by Bi<sub>2</sub>O<sub>3</sub> disperse and its native very high dielectric strength.</p></div>
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Dielectric characteristics such as dielectric constant (ε′), dielectric loss (ε″), dielectric loss tangent (tanδ) and real and imaginary parts of electrical modulus (Μ′ and Μ″), and ac electrical conductivity (σac) of Au/ Polyvinyl Alcohol (PVA) (Bi2O3-dispersed)/n-Si structures have been investigated by using admittance measurements. Results show that the ε′ values of Au/PVA/n-Si with Bi2O3-dispersed PVA interfacial layer are very higher compared with those with pure and other dopant/mixture's of PVA. Thus, PVA is made very compatible for device applications with the enhanced dielectric properties by Bi2O3 disperse and its native very high dielectric strength.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12012" xmlns="http://purl.org/rss/1.0/"><title>SiC Matrix Structure–Function Composites Prepared by Pressureless Sintering and Their Microwave Attenuation Property in the X Band</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12012</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">SiC Matrix Structure–Function Composites Prepared by Pressureless Sintering and Their Microwave Attenuation Property in the X Band</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Zehua Zhou, Zehua Wang, Ying Ding, Yu Yi, Shaoqun Jiang, Weihua Zhao, Shouhong Tan, Dongliang Jiang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T11:26:01.003152-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12012</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12012</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12012</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>For developing excellent microwave attenuation materials in a wide band, two series of SiC-C (graphite) composites with different C additions were fabricated by pressureless sintering, using α-SiC and β-SiC green powder, respectively. β-SBC composites were more suitable for microwave attenuation materials than α-SBC composites. β-SiC composites with 3 wt% C additions exhibited the best microwave absorption: The most significant microwave attenuation was −40.5 dB, and most other attenuations were above −30 dB in the whole X band. The composites were prepared with cost-effective and easily controllable manufacturing process and can be considered as structure–function materials for particular applications.</p></div>
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For developing excellent microwave attenuation materials in a wide band, two series of SiC-C (graphite) composites with different C additions were fabricated by pressureless sintering, using α-SiC and β-SiC green powder, respectively. β-SBC composites were more suitable for microwave attenuation materials than α-SBC composites. β-SiC composites with 3 wt% C additions exhibited the best microwave absorption: The most significant microwave attenuation was −40.5 dB, and most other attenuations were above −30 dB in the whole X band. The composites were prepared with cost-effective and easily controllable manufacturing process and can be considered as structure–function materials for particular applications.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12016" xmlns="http://purl.org/rss/1.0/"><title>Synthesis of Ultrafine Hafnium Diboride Powders Using Solution-Based Processing and Spark Plasma Sintering</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12016</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Synthesis of Ultrafine Hafnium Diboride Powders Using Solution-Based Processing and Spark Plasma Sintering</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hailong Wang, Sea-Hoon Lee, Hai-Doo Kim, Hyeon-Cheol Oh</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T11:25:54.745619-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12016</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12016</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12016</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Ultrafine hafnium diboride (HfB<sub>2</sub>) powders were synthesized by the boro/carborthermal reduction process. Fine-scale mixing of the reactants was achieved by solution-based processing using hafnium oxychloride (HfOCl<sub>2</sub>·8H<sub>2</sub>O) and phenolic resin as the precursor of HfO<sub>2</sub> and carbon respectively. The heat treatment was completed at a temperature range 1300–1500°C for 1h using spark plasma sintering (SPS) apparatus. The crystallite sizes of the synthesized powders were small (&lt;500 nm) and the oxygen content was low (0.85 wt%). The grain growth of HfB<sub>2</sub> could be effectively suppressed using SPS due to the fast heating rate. The effects of temperature and holding time on the synthesis of ultrafine HfB<sub>2</sub> powders were discussed.</p></div>
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Ultrafine hafnium diboride (HfB2) powders were synthesized by the boro/carborthermal reduction process. Fine-scale mixing of the reactants was achieved by solution-based processing using hafnium oxychloride (HfOCl2·8H2O) and phenolic resin as the precursor of HfO2 and carbon respectively. The heat treatment was completed at a temperature range 1300–1500°C for 1h using spark plasma sintering (SPS) apparatus. The crystallite sizes of the synthesized powders were small (&lt;500 nm) and the oxygen content was low (0.85 wt%). The grain growth of HfB2 could be effectively suppressed using SPS due to the fast heating rate. The effects of temperature and holding time on the synthesis of ultrafine HfB2 powders were discussed.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12014" xmlns="http://purl.org/rss/1.0/"><title>A Si–SiC Oxidation-resistant Coating for Carbon/Carbon Composites by Hot-pressing Reaction Technique</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12014</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A Si–SiC Oxidation-resistant Coating for Carbon/Carbon Composites by Hot-pressing Reaction Technique</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Fu Qiangang, Cao Cuiwei, Li Hejun, Tao Jun, Li Kezhi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T11:25:42.88691-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12014</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12014</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12014</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A Si–SiC coating was prepared by hot-pressing reactive sintering (HPRS) technique for protecting carbon/carbon (C/C) composites against oxidation. The Si–SiC coating has a dense and crack-free structure with a thickness of 70–90 μm. The Si–SiC coating by HPRS has a higher SiC content and lower Si content than the coating by pressure-less reactive sintering (PRS). It also exhibits better oxidation-protective ability than that prepared by PRS. With hot-pressing, the flexural strength of the Si–SiC coated C/C composites decreases from 121 MPa to 99 MPa, and the interface bonding strength increases from 6 MPa to 10 MPa.</p></div>
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A Si–SiC coating was prepared by hot-pressing reactive sintering (HPRS) technique for protecting carbon/carbon (C/C) composites against oxidation. The Si–SiC coating has a dense and crack-free structure with a thickness of 70–90 μm. The Si–SiC coating by HPRS has a higher SiC content and lower Si content than the coating by pressure-less reactive sintering (PRS). It also exhibits better oxidation-protective ability than that prepared by PRS. With hot-pressing, the flexural strength of the Si–SiC coated C/C composites decreases from 121 MPa to 99 MPa, and the interface bonding strength increases from 6 MPa to 10 MPa.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12013" xmlns="http://purl.org/rss/1.0/"><title>Fabrication of Mn–Co Spinel Coatings on Crofer 22 APU Stainless Steel by Electrophoretic Deposition for Interconnect Applications in Solid Oxide Fuel Cells</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12013</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Fabrication of Mn–Co Spinel Coatings on Crofer 22 APU Stainless Steel by Electrophoretic Deposition for Interconnect Applications in Solid Oxide Fuel Cells</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yong Zhang, Athar Javed, Mengmeng Zhou, Shuquan Liang, Ping Xiao</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T11:25:34.859671-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12013</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12013</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12013</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>This study investigates the microstructure, oxidation kinetics, and electrical behavior of Mn–Co spinel coating for interconnect applications in solid oxide fuel cells. A relatively dense, uniform, and well-adherent Mn–Co (Mn<sub>1.5</sub>Co<sub>1.5</sub>O<sub>4</sub>) spinel coating with good oxidation resistance and stable conductivity was successfully prepared on the surface of Crofer 22 APU stainless steel using electrophoretic deposition followed by sintering at 1150°C. During further thermal treatment at 800°C, the chromium oxide (Cr<sub>2</sub>O<sub>3</sub>) sublayer formed at the substrate/coating interface during sintering showed a very slow growth, and no chromium penetration was detected in the Mn–Co coating. The oxidation kinetics of the Mn–Co-coated substrate obeyed the parabolic law with the a parabolic rate constant <em>k</em><sub>p</sub> of 5.20 × 10<sup>−15</sup> g<sup>2</sup>/cm<sup>4</sup>/s, which was 1–2 orders of magnitude lower than that of the uncoated Crofer 22 APU stainless steel substrate. For oxidation (at 800°C) times ≥50 h, the area-specific resistance of the Mn–Co-coated Crofer 22 APU substrate became ~17 mΩ·cm<sup>2</sup> and was almost constant after further oxidation.</p></div>
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This study investigates the microstructure, oxidation kinetics, and electrical behavior of Mn–Co spinel coating for interconnect applications in solid oxide fuel cells. A relatively dense, uniform, and well-adherent Mn–Co (Mn1.5Co1.5O4) spinel coating with good oxidation resistance and stable conductivity was successfully prepared on the surface of Crofer 22 APU stainless steel using electrophoretic deposition followed by sintering at 1150°C. During further thermal treatment at 800°C, the chromium oxide (Cr2O3) sublayer formed at the substrate/coating interface during sintering showed a very slow growth, and no chromium penetration was detected in the Mn–Co coating. The oxidation kinetics of the Mn–Co-coated substrate obeyed the parabolic law with the a parabolic rate constant kp of 5.20 × 10−15 g2/cm4/s, which was 1–2 orders of magnitude lower than that of the uncoated Crofer 22 APU stainless steel substrate. For oxidation (at 800°C) times ≥50 h, the area-specific resistance of the Mn–Co-coated Crofer 22 APU substrate became ~17 mΩ·cm2 and was almost constant after further oxidation.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12022" xmlns="http://purl.org/rss/1.0/"><title>Improved Thermal Stress Resistance Parameters Considering Temperature Gradients for Bricks in Refractory Linings</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12022</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Improved Thermal Stress Resistance Parameters Considering Temperature Gradients for Bricks in Refractory Linings</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Erwan Brochen, Jürgen Pötschke, Christos G. Aneziris</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T11:20:19.146722-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12022</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12022</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12022</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The thermal stress resistance (TSR) parameters available in the literature are basically “figures of merit” that should help for the selection of materials for engineering design involving thermal stress fracture. However, they are based on very simplified models. For instance, they neglect or simplify the thermal gradient or rather the stress field that actually exist in practice. The state of stress was analytically calculated and the results implemented in the established thermal stress fracture parameters (R, R″) and damage parameter (<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1111/ijac.12022/asset/equation/ijac12022-math-0001.gif?v=1&amp;t=hi4mvwkw&amp;s=3f77670a6919196d4037265aa7af95f4e74c17d2" class="inlineGraphic"/>). For each of them, an analytical solution and an approximation were derived. The reviewed TSR parameters allow a clearly improved prediction of the resistance to thermal shock for bricks in refractory linings and facilitate the classification of industrial refractories.</p></div>
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The thermal stress resistance (TSR) parameters available in the literature are basically “figures of merit” that should help for the selection of materials for engineering design involving thermal stress fracture. However, they are based on very simplified models. For instance, they neglect or simplify the thermal gradient or rather the stress field that actually exist in practice. The state of stress was analytically calculated and the results implemented in the established thermal stress fracture parameters (R, R″) and damage parameter (R″″). For each of them, an analytical solution and an approximation were derived. The reviewed TSR parameters allow a clearly improved prediction of the resistance to thermal shock for bricks in refractory linings and facilitate the classification of industrial refractories.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12008" xmlns="http://purl.org/rss/1.0/"><title>Preparation of Fe3Si-Al2O3 Nanocomposite Powders by Mechanochemical Reaction of Fe3O4-Si-Al Powder Mixtures</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12008</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Preparation of Fe3Si-Al2O3 Nanocomposite Powders by Mechanochemical Reaction of Fe3O4-Si-Al Powder Mixtures</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jiangang Jia, Tieming Guo, Shufang Ren, Jinjun Lu, Qin Ma</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-22T10:48:57.822358-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12008</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12008</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12008</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Phase evolution and morphology of Fe<sub>3</sub>O<sub>4</sub>-Si-Al powder mixtures during ball milling from 30 min to 20 h were investigated. A 3-h critical milling was necessary for the occurrence of mechanically activated combustion reaction. The reaction results in the formation of Fe (Si), Fe<sub>3</sub>Si, and α-Al<sub>2</sub>O<sub>3</sub>. During ball milling from 3 to 20 h, Fe (Si) and Fe<sub>3</sub>Si were combined into disordered Fe<sub>3</sub>Si intermetallic and Fe<sub>3</sub>Si-Al<sub>2</sub>O<sub>3</sub> composite powder was formed. The presence of <em>in situ</em> formed alumina leads to a decrease in crystallite and particle sizes. The Fe<sub>3</sub>Si-Al<sub>2</sub>O<sub>3</sub> particles after milling for 20 h had a crystalline size of 10~12 nm.</p></div>
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Phase evolution and morphology of Fe3O4-Si-Al powder mixtures during ball milling from 30 min to 20 h were investigated. A 3-h critical milling was necessary for the occurrence of mechanically activated combustion reaction. The reaction results in the formation of Fe (Si), Fe3Si, and α-Al2O3. During ball milling from 3 to 20 h, Fe (Si) and Fe3Si were combined into disordered Fe3Si intermetallic and Fe3Si-Al2O3 composite powder was formed. The presence of in situ formed alumina leads to a decrease in crystallite and particle sizes. The Fe3Si-Al2O3 particles after milling for 20 h had a crystalline size of 10~12 nm.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12007" xmlns="http://purl.org/rss/1.0/"><title>Improved Photoluminescence Property of YBO3:Eu3+ Phosphor by Structure Tailoring</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12007</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Improved Photoluminescence Property of YBO3:Eu3+ Phosphor by Structure Tailoring</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dalai Jin, Jingjing Yang, Xiang Miao, Lina Wang, Longcheng Wang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-22T10:48:52.688456-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12007</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12007</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12007</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>YBO<sub>3</sub>:Eu<sup>3+</sup> microspheres were synthesized by a hydrothermal method. Size and surface morphology of the spheres were tailored by ion-adding. Phase identification, morphology observation, and photoluminescence (PL) performance of the YBO<sub>3</sub>:Eu<sup>3+</sup> microspheres were characterized byX-ray diffraction (XRD), field-emission scanning electron microscopy (FESEM), and PL spectrophotometer, respectively. Moderate particles with enlarged size and perfect surface were achieved by adding Li<sup>+</sup> ion or/and Mg<sup>2+</sup> ion. PL emissions of such YBO<sub>3</sub>:Eu<sup>3+</sup> phosphors were enhanced. Significantly improved PL intensity was achieved when 1% Li<sup>+</sup> ion and 5% Mg<sup>2+</sup> ion were added, which was nearly doubled compared with the reference sample.</p></div>
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YBO3:Eu3+ microspheres were synthesized by a hydrothermal method. Size and surface morphology of the spheres were tailored by ion-adding. Phase identification, morphology observation, and photoluminescence (PL) performance of the YBO3:Eu3+ microspheres were characterized byX-ray diffraction (XRD), field-emission scanning electron microscopy (FESEM), and PL spectrophotometer, respectively. Moderate particles with enlarged size and perfect surface were achieved by adding Li+ ion or/and Mg2+ ion. PL emissions of such YBO3:Eu3+ phosphors were enhanced. Significantly improved PL intensity was achieved when 1% Li+ ion and 5% Mg2+ ion were added, which was nearly doubled compared with the reference sample.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12029" xmlns="http://purl.org/rss/1.0/"><title>Amorphous Ternary Ceramics Instability Below 450°C: Nano-Scale Arguments from the Lattice Compatibility Theory (LCT)</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12029</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Amorphous Ternary Ceramics Instability Below 450°C: Nano-Scale Arguments from the Lattice Compatibility Theory (LCT)</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Karem Boubaker, Mosbah Amlouk</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-21T14:56:18.861712-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12029</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12029</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12029</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>In this paper, we present some elements of the lattice compatibility theory (LCT) as plausible explanations to the problem of instability of some ternary ceramics under some circumstances. Particular attention is paid to ceramics nano-scale patterns.</p></div>
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In this paper, we present some elements of the lattice compatibility theory (LCT) as plausible explanations to the problem of instability of some ternary ceramics under some circumstances. Particular attention is paid to ceramics nano-scale patterns.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12021" xmlns="http://purl.org/rss/1.0/"><title>Reducing Loss Tangent by Controlling Microstructure and Electrical Responses in CaCu3Ti4O12 Ceramics Prepared by a Simple Combustion Method</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12021</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Reducing Loss Tangent by Controlling Microstructure and Electrical Responses in CaCu3Ti4O12 Ceramics Prepared by a Simple Combustion Method</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Prasit Thongbai, Supree Pinitsoontorn, Vittaya Amornkitbamrung, Teerapon Yamwong, Santi Maensiri, Prinya Chindaprasirt</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-21T14:56:14.673581-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12021</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12021</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12021</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The dielectric and electrical properties of CaCu<sub>3</sub>Ti<sub>4</sub>O<sub>12</sub> ceramics prepared by a simple combustion method were investigated. Fine-grained CaCu<sub>3</sub>Ti<sub>4</sub>O<sub>12</sub> ceramics exhibited good dielectric properties and temperature stability. Very low loss tangents of 0.020–0.016 and high dielectric constant of 5776–6406 (at 1 kHz and 20°C) with temperature coefficient less than ±15% in the temperature range of −70 to 90°C were observed. Dielectric relaxation processes were observed in large-grained CaCu<sub>3</sub>Ti<sub>4</sub>O<sub>12</sub> ceramics. The dielectric relaxation in the temperature range of 60–150°C may be associated with sample–electrode contact. The relaxation in temperatures below −40°C is related to the electrical response at grain boundaries.</p></div>
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The dielectric and electrical properties of CaCu3Ti4O12 ceramics prepared by a simple combustion method were investigated. Fine-grained CaCu3Ti4O12 ceramics exhibited good dielectric properties and temperature stability. Very low loss tangents of 0.020–0.016 and high dielectric constant of 5776–6406 (at 1 kHz and 20°C) with temperature coefficient less than ±15% in the temperature range of −70 to 90°C were observed. Dielectric relaxation processes were observed in large-grained CaCu3Ti4O12 ceramics. The dielectric relaxation in the temperature range of 60–150°C may be associated with sample–electrode contact. The relaxation in temperatures below −40°C is related to the electrical response at grain boundaries.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12020" xmlns="http://purl.org/rss/1.0/"><title>The Effect of pH Value on Phase Transformation of Calcium Phosphate Cement</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12020</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">The Effect of pH Value on Phase Transformation of Calcium Phosphate Cement</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hsin-Chung Cheng, Kuo-Tien Chu, Nai-Cia Teng, Hsien-Lung Tsai, Keng-Liang Ou, Shih-Fu Ou</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-21T14:56:08.501029-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12020</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12020</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12020</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The effects of various pH values of sodium phosphate buffer solution (PBS), 4.0, 6.0, 8.0, and 9.0 on calcium phosphate cement (CPC) prepared by mixing monocalcium phosphate monohydrate (MCPM), calcium carbonate, and PBS were studied. The phase evolution takes place in three steps: Firstly, the MCPM and calcium carbonate crystals dissolve in the PBS and precipitate in the form of DCPD crystals. Then, after 12 h, DCPD begins to convert to amorphous calcium phosphate (ACP). Finally, the metastable ACP phase converts into stable CDHA. With an increase in the pH of the PBS, the CDHA content in the CPC increased.</p></div>
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The effects of various pH values of sodium phosphate buffer solution (PBS), 4.0, 6.0, 8.0, and 9.0 on calcium phosphate cement (CPC) prepared by mixing monocalcium phosphate monohydrate (MCPM), calcium carbonate, and PBS were studied. The phase evolution takes place in three steps: Firstly, the MCPM and calcium carbonate crystals dissolve in the PBS and precipitate in the form of DCPD crystals. Then, after 12 h, DCPD begins to convert to amorphous calcium phosphate (ACP). Finally, the metastable ACP phase converts into stable CDHA. With an increase in the pH of the PBS, the CDHA content in the CPC increased.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12015" xmlns="http://purl.org/rss/1.0/"><title>Preparation, Characterization, and Thermophysical Properties of (La0.95Sr0.05)2Ce2O6.95 Ceramic for Thermal Barrier Coatings</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12015</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Preparation, Characterization, and Thermophysical Properties of (La0.95Sr0.05)2Ce2O6.95 Ceramic for Thermal Barrier Coatings</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Zhang Hong-Song, Lv Jian-Guo, Li Gang, Chen Xiao-Ge, Wang Xin-Li</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-21T14:56:03.492143-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12015</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12015</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12015</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The La<sub>2</sub>Ce<sub>2</sub>O<sub>7</sub> powder doped with Sr was synthesized by sol-gel method in this study and its dense bulk samples were also prepared by pressureless-sintered at 1600°C for 10 h. Its phase composition, microstructure, and thermophysical property were investigated. Results reveal that pure (La<sub>0.95</sub>Sr<sub>0.05</sub>)<sub>2</sub>Ce<sub>2</sub>O<sub>6.95</sub> with single fluorite structure was successfully synthesized. Microstructure of bulk sample is dense. Its thermal expansion coefficient is higher than that of Y<sub>2</sub>O<sub>3</sub>-stabilized ZrO<sub>2</sub> (YSZ) and its thermal conductivity is lower than that of YSZ. These results show that (La<sub>0.95</sub>Sr<sub>0.05</sub>)<sub>2</sub>Ce<sub>2</sub>O<sub>6.95</sub> ceramic can be explored as the candidate material for thermal barrier coatings.</p></div>
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The La2Ce2O7 powder doped with Sr was synthesized by sol-gel method in this study and its dense bulk samples were also prepared by pressureless-sintered at 1600°C for 10 h. Its phase composition, microstructure, and thermophysical property were investigated. Results reveal that pure (La0.95Sr0.05)2Ce2O6.95 with single fluorite structure was successfully synthesized. Microstructure of bulk sample is dense. Its thermal expansion coefficient is higher than that of Y2O3-stabilized ZrO2 (YSZ) and its thermal conductivity is lower than that of YSZ. These results show that (La0.95Sr0.05)2Ce2O6.95 ceramic can be explored as the candidate material for thermal barrier coatings.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12042" xmlns="http://purl.org/rss/1.0/"><title>SnO2 Nanosheet–assembled Graded Continuous Film</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12042</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">SnO2 Nanosheet–assembled Graded Continuous Film</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yoshitake Masuda, Kazumi Kato</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-21T13:10:43.317155-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12042</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12042</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12042</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>SnO<sub>2</sub> nanosheet–assembled graded continuous films were successfully fabricated in aqueous solutions containing SnF<sub>2</sub> of 250 m<em>M</em> at 90°C. Thickness reached 1200 nm after immersion for 24 h. The nanosheets were 100–500 nm in in-plane sheet size and 5–20 nm in thickness. The graded structures were caused by gradual change in supersaturation degree of the solutions. The films had <em>a</em>-axis orientation, antireflective effect, band gap of 3.63 eV, and superhydrophilic surfaces. In contrast, the films immersed for 20 m showed band gap of 4.04 eV and contact angle of 58°.</p></div>
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SnO2 nanosheet–assembled graded continuous films were successfully fabricated in aqueous solutions containing SnF2 of 250 mM at 90°C. Thickness reached 1200 nm after immersion for 24 h. The nanosheets were 100–500 nm in in-plane sheet size and 5–20 nm in thickness. The graded structures were caused by gradual change in supersaturation degree of the solutions. The films had a-axis orientation, antireflective effect, band gap of 3.63 eV, and superhydrophilic surfaces. In contrast, the films immersed for 20 m showed band gap of 4.04 eV and contact angle of 58°.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12043" xmlns="http://purl.org/rss/1.0/"><title>The Effect of Zirconium Carbide on Ablation of SiC-Coated Carbon/Silicon Carbide Composites Under an Oxy-Acetylene Flame</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12043</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">The Effect of Zirconium Carbide on Ablation of SiC-Coated Carbon/Silicon Carbide Composites Under an Oxy-Acetylene Flame</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Xiang Yang, Li Wei, Wang Song, Chen Zhao-Hui</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-21T13:10:29.891666-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12043</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12043</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12043</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>To improve the ablation resistance of PIP-C/<span class="fixed-roman">SiC</span> composites, zirconium carbide (<span class="fixed-roman">ZrC</span>)-modified <span class="fixed-roman">SiC</span> coating was prepared by chemical vapor deposition combined with slurry painting, then the ablation capability of the coated composites was tested under an oxy-acetylene torch. Compared with the uncoated composites, linear and mass ablation rates of the coated composites decreased by 73.6% and 76.4%, respectively. The formation of zirconia from the oxidation of <span class="fixed-roman">ZrC</span> improved the ablation resistance of the composites because of anti-oxidation performance, which absorbed heat from the flame and reduced erosive attack to <span class="fixed-roman">C</span>/<span class="fixed-roman">SiC</span> composites. Zirconia also acted as an accelerator for carbon fiber oxidation as it reacted with carbon during ablation. The heterogeneous reactions controlled the ablation of the composites.</p></div>
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To improve the ablation resistance of PIP-C/SiC composites, zirconium carbide (ZrC)-modified SiC coating was prepared by chemical vapor deposition combined with slurry painting, then the ablation capability of the coated composites was tested under an oxy-acetylene torch. Compared with the uncoated composites, linear and mass ablation rates of the coated composites decreased by 73.6% and 76.4%, respectively. The formation of zirconia from the oxidation of ZrC improved the ablation resistance of the composites because of anti-oxidation performance, which absorbed heat from the flame and reduced erosive attack to C/SiC composites. Zirconia also acted as an accelerator for carbon fiber oxidation as it reacted with carbon during ablation. The heterogeneous reactions controlled the ablation of the composites.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12006" xmlns="http://purl.org/rss/1.0/"><title>Study of Screen-Printed PZT Cantilevers Both Self-Actuated and Self-Read-Out</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12006</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Study of Screen-Printed PZT Cantilevers Both Self-Actuated and Self-Read-Out</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Riadh Lakhmi, Hélène Debeda, Mario Maglione, Isabelle Dufour, Claude Lucat</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-21T12:41:34.023519-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12006</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12006</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12006</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Usually, resonating cantilevers come from silicon technology and are activated with pure bending mode. In this work, we suggest to combine high-sensitive cantilever structure with both self-actuated and self-read-out piezoelectric thick-film for high electrical–mechanical coupling. This cantilever is realized through screen-printing deposition associated with a sacrificial layer. It is composed of a PZT layer between two gold electrodes. Optimum performances of piezoelectric ceramics generally imply the use of mechanical pressure and very high sintering temperature that are not compatible with the screen-printing process. Addition of eutectic composition Li<sub>2</sub>CO<sub>3</sub>-Bi<sub>2</sub>O<sub>3</sub>-CuO or borosilicate glass-frit to PZT powder and application of isostatic pressure improve the sintering at a given temperature. Firing temperature of 850°C, 900°C, and 950°C is tested. Microstructural, electrical and mechanical characterizations are achieved. In addition to the bending mode, the in-plane 31-longitudinal vibration mode and the out-of-plane 33-thickness resonance mode are revealed. Correlations between experimental results and modeling of the different vibration modes are established. The piezoelectric parameters of PZT cantilevers approach those of ceramics. Quality factors between 300 and 400 associated with the unusual 31-longitudinal mode make screen-printed PZT cantilevers good candidates for detection in liquid and gaseous media.</p></div>
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Usually, resonating cantilevers come from silicon technology and are activated with pure bending mode. In this work, we suggest to combine high-sensitive cantilever structure with both self-actuated and self-read-out piezoelectric thick-film for high electrical–mechanical coupling. This cantilever is realized through screen-printing deposition associated with a sacrificial layer. It is composed of a PZT layer between two gold electrodes. Optimum performances of piezoelectric ceramics generally imply the use of mechanical pressure and very high sintering temperature that are not compatible with the screen-printing process. Addition of eutectic composition Li2CO3-Bi2O3-CuO or borosilicate glass-frit to PZT powder and application of isostatic pressure improve the sintering at a given temperature. Firing temperature of 850°C, 900°C, and 950°C is tested. Microstructural, electrical and mechanical characterizations are achieved. In addition to the bending mode, the in-plane 31-longitudinal vibration mode and the out-of-plane 33-thickness resonance mode are revealed. Correlations between experimental results and modeling of the different vibration modes are established. The piezoelectric parameters of PZT cantilevers approach those of ceramics. Quality factors between 300 and 400 associated with the unusual 31-longitudinal mode make screen-printed PZT cantilevers good candidates for detection in liquid and gaseous media.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12005" xmlns="http://purl.org/rss/1.0/"><title>Determination of Density Variation and Microstructure in Reaction-sintered SiC Ceramics Using Ultrasonic Time-of-Flight</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12005</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Determination of Density Variation and Microstructure in Reaction-sintered SiC Ceramics Using Ultrasonic Time-of-Flight</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Manasa Kesharaju, Romesh Nagarajah</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-21T12:41:28.793498-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12005</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12005</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12005</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Ultrasonic time-of-flight (TOF) is investigated as a predictor of density variation across reaction-sintered silicon carbide (SiC) ceramics. The importance of this research is heightened by the fact that the reaction-sintered SiC ceramic tiles being investigated are manufactured using the reaction sintering process that involves the infusion of liquid silicon into a porous ceramic preform. This can potentially lead to the formation of islands of free silicon, small closed areas of un-sintered silicon material as well as conventional porosity. All these defects can result in local variations of density which cannot be detected by conventional bulk density measurement techniques. To study the microstructural differences, the porosity dependence of ultrasonic TOF of the reflected signals was investigated to establish a correlation between the velocity and density across the ceramic tile that aids in characterizing the material. The data suggest that for these ceramic tiles, TOF C-scan mapping surfs as a much better indicator of sample homogeneity than the amplitude of the back wall echo. At the current time, ceramic tiles are inspected offline and this takes time and effort and is very expensive. In particular, this study contains the procedure followed to establish a quantitative method to quantify density variation across selected ceramic tile.</p></div>
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Ultrasonic time-of-flight (TOF) is investigated as a predictor of density variation across reaction-sintered silicon carbide (SiC) ceramics. The importance of this research is heightened by the fact that the reaction-sintered SiC ceramic tiles being investigated are manufactured using the reaction sintering process that involves the infusion of liquid silicon into a porous ceramic preform. This can potentially lead to the formation of islands of free silicon, small closed areas of un-sintered silicon material as well as conventional porosity. All these defects can result in local variations of density which cannot be detected by conventional bulk density measurement techniques. To study the microstructural differences, the porosity dependence of ultrasonic TOF of the reflected signals was investigated to establish a correlation between the velocity and density across the ceramic tile that aids in characterizing the material. The data suggest that for these ceramic tiles, TOF C-scan mapping surfs as a much better indicator of sample homogeneity than the amplitude of the back wall echo. At the current time, ceramic tiles are inspected offline and this takes time and effort and is very expensive. In particular, this study contains the procedure followed to establish a quantitative method to quantify density variation across selected ceramic tile.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12032" xmlns="http://purl.org/rss/1.0/"><title>Production of Al2O3-Stabilized Tetragonal ZrO2 Nanoparticles for Thermal Barrier Coating</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12032</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Production of Al2O3-Stabilized Tetragonal ZrO2 Nanoparticles for Thermal Barrier Coating</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Arumugam Karthik, Palanisamy Manivasakan, Sundaramoorthy Arunmetha, Rathinam Yuvakkumar, Venkatachalam Rajendran</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-04T11:46:38.863576-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12032</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12032</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12032</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Al<sub>2</sub>O<sub>3</sub>-stabilized tetragonal ZrO<sub>2</sub> nanoparticles were obtained through hot-air spray pyrolysis and characterized after postsynthesized treatments. The produced nanoparticles were 26 nm in size with surface area of 59 m<sup>2</sup>/g. A multilayer thermal barrier coating of nanostructured Al<sub>2</sub>O<sub>3</sub>-ZrO<sub>2</sub>-embedded silicate was applied to the mild steel (EN3) specimen using spin-coating technique and characterized comprehensively employing X-ray diffraction and scanning electron microscope. The Al<sub>2</sub>O<sub>3</sub>-stabilized ZrO<sub>2</sub> with silicate matrix facilitates the formation of zirconium silicate nanostructured surface-protective coating on EN3 specimen. The Al<sub>2</sub>O<sub>3</sub>-ZrO<sub>2</sub>/SiO<sub>2</sub> matrix-based hybrid inorganic coating shows effective thermal barrier for EN3 after firing at a high temperature of 600°C.</p></div>
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Al2O3-stabilized tetragonal ZrO2 nanoparticles were obtained through hot-air spray pyrolysis and characterized after postsynthesized treatments. The produced nanoparticles were 26 nm in size with surface area of 59 m2/g. A multilayer thermal barrier coating of nanostructured Al2O3-ZrO2-embedded silicate was applied to the mild steel (EN3) specimen using spin-coating technique and characterized comprehensively employing X-ray diffraction and scanning electron microscope. The Al2O3-stabilized ZrO2 with silicate matrix facilitates the formation of zirconium silicate nanostructured surface-protective coating on EN3 specimen. The Al2O3-ZrO2/SiO2 matrix-based hybrid inorganic coating shows effective thermal barrier for EN3 after firing at a high temperature of 600°C.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12035" xmlns="http://purl.org/rss/1.0/"><title>Effect of Aluminum Content on Mechanical Properties and Thermal Conductivities of Sintered Reaction-Bonded Silicon Nitride</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12035</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of Aluminum Content on Mechanical Properties and Thermal Conductivities of Sintered Reaction-Bonded Silicon Nitride</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dai Kusano, Hideki Hyuga, You Zhou, Kiyoshi Hirao</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-04T11:45:34.174123-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12035</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12035</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12035</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A systematic study was conducted of the effect of <span class="fixed-roman">Al</span> impurities on the mechanical and thermal properties of sintered reaction-bonded silicon nitrides (SRBSNs). 2 mol.% Y<sub>2</sub>O<sub>3</sub> and 5 mol.% MgSiN<sub>2</sub> were added as sintering aids to high-purity raw <span class="fixed-roman">Si</span> powder, followed by respective additions of 0, 0.01, 0.1, 0.2, and 0.4 mass% of <span class="fixed-roman">Al</span> relative to <span class="fixed-roman">Si</span>. The prepared powder mixes were press formed and nitrided in a 0.1 MPa nitrogen atmosphere at 1400°C for 8 h. Postsintering of the nitrides was conducted under a pressurized nitrogen atmosphere of 0.9 MPa at 1900°C for 6 h. The SRBSN specimens exhibited hardly any difference in their four-point bending strength, which ranged from 800 to 850 MPa. However, their fracture toughness clearly decreased with increasing additive <span class="fixed-roman">Al</span> content. This is thought to be due to a reduction in the proportion of coarse prismatic grains improving the toughness with increasing additive <span class="fixed-roman">Al</span> content. A significant reduction in the thermal conductivity was also observed with increasing additive <span class="fixed-roman">Al</span> content. This is conjectured to be due to the formation of SiAlON through a substituted solid solution of aluminum (<span class="fixed-roman">Al</span>) and oxygen (<span class="fixed-roman">O</span>) in β-Si<sub>3</sub>N<sub>4</sub> crystals. An inductively coupled plasma and hot gas extraction method were employed to directly analyze <span class="fixed-roman">Al</span> and <span class="fixed-roman">O</span> in β-Si<sub>3</sub>N<sub>4</sub> particles. Approximately half of the additive <span class="fixed-roman">Al</span> was confirmed to be in solid solution in β-Si<sub>3</sub>N<sub>4</sub> particles along with the solid solution of <span class="fixed-roman">O</span> in a chemical formula that nearly corresponds to β-Si<sub>6–z</sub>Al<sub>z</sub>O<sub>z</sub>N<sub>8–z</sub>. The chemical analysis results give a <em>Z</em> value range of 0.0006–0.024.</p></div>
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A systematic study was conducted of the effect of Al impurities on the mechanical and thermal properties of sintered reaction-bonded silicon nitrides (SRBSNs). 2 mol.% Y2O3 and 5 mol.% MgSiN2 were added as sintering aids to high-purity raw Si powder, followed by respective additions of 0, 0.01, 0.1, 0.2, and 0.4 mass% of Al relative to Si. The prepared powder mixes were press formed and nitrided in a 0.1 MPa nitrogen atmosphere at 1400°C for 8 h. Postsintering of the nitrides was conducted under a pressurized nitrogen atmosphere of 0.9 MPa at 1900°C for 6 h. The SRBSN specimens exhibited hardly any difference in their four-point bending strength, which ranged from 800 to 850 MPa. However, their fracture toughness clearly decreased with increasing additive Al content. This is thought to be due to a reduction in the proportion of coarse prismatic grains improving the toughness with increasing additive Al content. A significant reduction in the thermal conductivity was also observed with increasing additive Al content. This is conjectured to be due to the formation of SiAlON through a substituted solid solution of aluminum (Al) and oxygen (O) in β-Si3N4 crystals. An inductively coupled plasma and hot gas extraction method were employed to directly analyze Al and O in β-Si3N4 particles. Approximately half of the additive Al was confirmed to be in solid solution in β-Si3N4 particles along with the solid solution of O in a chemical formula that nearly corresponds to β-Si6–zAlzOzN8–z. The chemical analysis results give a Z value range of 0.0006–0.024.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12031" xmlns="http://purl.org/rss/1.0/"><title>The Effect of Particle Size on the Mechanical and Microstructural Properties of Freeze-Casted Macroporous Hydroxyapatite Scaffolds</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12031</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">The Effect of Particle Size on the Mechanical and Microstructural Properties of Freeze-Casted Macroporous Hydroxyapatite Scaffolds</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ali Zamanian, Sajad Farhangdoust, Mana Yasaei, Mina Khorami, Masoud Hafezi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-04T11:45:25.244822-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12031</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12031</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12031</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Two different hydroxyapatites with the particle sizes of 3.9 and 1.69 μm were chosen. Slurries with initial hydroxyapatite concentration of 15 vol% were prepared. Different cooling rates from 2 to 14°C/min were utilized. The specimens were sintered at different temperatures of 1250–1350°C. The phase composition (by X-Ray Diffraction), microstructure (by Scanning Electron Microscopy), mechanical characteristics, and the porosity of sintered samples were assessed. The porosity of the sintered samples was in range of ~57–83%, and the compressive strength varied from ~1.7 to 15 MPa. The mechanical strength of the scaffolds increased as a function of cooling rate and sintering temperature.</p></div>
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Two different hydroxyapatites with the particle sizes of 3.9 and 1.69 μm were chosen. Slurries with initial hydroxyapatite concentration of 15 vol% were prepared. Different cooling rates from 2 to 14°C/min were utilized. The specimens were sintered at different temperatures of 1250–1350°C. The phase composition (by X-Ray Diffraction), microstructure (by Scanning Electron Microscopy), mechanical characteristics, and the porosity of sintered samples were assessed. The porosity of the sintered samples was in range of ~57–83%, and the compressive strength varied from ~1.7 to 15 MPa. The mechanical strength of the scaffolds increased as a function of cooling rate and sintering temperature.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02821.x" xmlns="http://purl.org/rss/1.0/"><title>Mechanochemical and Low-Temperature Synthesis of Nanocrystalline Fluorohydroxyapatite/Fluorapatite</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02821.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Mechanochemical and Low-Temperature Synthesis of Nanocrystalline Fluorohydroxyapatite/Fluorapatite</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Vukoman Jokanović, Božana Čolović, Nataša Jović, Branka Babić-Stojić, Bojan Jokanović</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-29T14:23:51.097759-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02821.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02821.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02821.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Low-temperature synthesis of fluorapatite/fluorohydroxyapatite with precursor mixture previously mechanochemically treated is described in this article. Ethylene vinylacetate/versatate copolymer as a surface active substance was mechanically treated to obtain a core-shell system with strongly controlled grain size. Despite usual behavior of mechanically activated systems, only an amorphous phase formed from precursor ions present in the mixture composed of <em>β</em>-<span class="fixed-roman">Ca</span><sub>2</sub><span class="fixed-roman">P</span><sub>2</sub><span class="fixed-roman">O</span><sub>7</sub>, <span class="fixed-roman">CaCO</span><sub>3</sub>, <span class="fixed-roman">CaF</span><sub>2</sub>, and unreacted <span class="fixed-roman">Ca</span>(<span class="fixed-roman">OH</span>)<sub>2</sub> was obtained during milling for 5 min to 8 h. The mixture contained depots of labile F<sup>−</sup> ions conserved in micelles cages, which are useful for teeth protection from carries. For transformation of these amorphous phases into fluorapatite, an additional low thermal treatment was necessary. The mechanism of the precursor mixture transformation into fluorapatite during milling and thermal treatment was investigated using FTIR spectroscopy and X-ray diffraction. The morphology and size distribution of the obtained powders was studied using SEM and TEM.</p></div>
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Low-temperature synthesis of fluorapatite/fluorohydroxyapatite with precursor mixture previously mechanochemically treated is described in this article. Ethylene vinylacetate/versatate copolymer as a surface active substance was mechanically treated to obtain a core-shell system with strongly controlled grain size. Despite usual behavior of mechanically activated systems, only an amorphous phase formed from precursor ions present in the mixture composed of β-Ca2P2O7, CaCO3, CaF2, and unreacted Ca(OH)2 was obtained during milling for 5 min to 8 h. The mixture contained depots of labile F− ions conserved in micelles cages, which are useful for teeth protection from carries. For transformation of these amorphous phases into fluorapatite, an additional low thermal treatment was necessary. The mechanism of the precursor mixture transformation into fluorapatite during milling and thermal treatment was investigated using FTIR spectroscopy and X-ray diffraction. The morphology and size distribution of the obtained powders was studied using SEM and TEM.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12024" xmlns="http://purl.org/rss/1.0/"><title>Novel Layered Hydroxyapatite/Tri-Calcium Phosphate–Zirconia Scaffold Composite with High Bending Strength for Load-Bearing Bone Implant Application</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12024</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Novel Layered Hydroxyapatite/Tri-Calcium Phosphate–Zirconia Scaffold Composite with High Bending Strength for Load-Bearing Bone Implant Application</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jing-Zhou Yang, Rumana Sultana, Xiao-Zhi Hu, Paul Ichim</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-18T11:26:51.840342-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12024</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12024</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12024</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The integration of biological and mechanical requirements remains a challenge in developing porous hydroxyapatite (HA) and tri-calcium phosphate (TCP) scaffolds for load-bearing bone implant application. With the newly developed slip-deposition and coating-substrate co-sintering technique, a strong layered HA/TCP-zirconia scaffold composite structure was successfully fabricated. The bending strength (321 MPa) of this composite can match upper strength limit of the natural compact bone. The HA-based scaffold coating has multiple scale porous structures with pore size ranging 1–10 and 20–50 μm. The zirconia-based substrate is also porous with submicropores. Focus ion beam micrographs show most of the micropores in the coating are interconnected. Microindentation and primarily adhesive strength tests demonstrate that the scaffold coating strongly bonds with the zirconia based substrate. <em>In vitro</em> cell culture study indicates that the coatings have no cytotoxicity. It is evident that the strong layered HA–zirconia scaffold composite offers new implant options for bone repairs requiring immediate load bearing capacity.</p></div>
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The integration of biological and mechanical requirements remains a challenge in developing porous hydroxyapatite (HA) and tri-calcium phosphate (TCP) scaffolds for load-bearing bone implant application. With the newly developed slip-deposition and coating-substrate co-sintering technique, a strong layered HA/TCP-zirconia scaffold composite structure was successfully fabricated. The bending strength (321 MPa) of this composite can match upper strength limit of the natural compact bone. The HA-based scaffold coating has multiple scale porous structures with pore size ranging 1–10 and 20–50 μm. The zirconia-based substrate is also porous with submicropores. Focus ion beam micrographs show most of the micropores in the coating are interconnected. Microindentation and primarily adhesive strength tests demonstrate that the scaffold coating strongly bonds with the zirconia based substrate. In vitro cell culture study indicates that the coatings have no cytotoxicity. It is evident that the strong layered HA–zirconia scaffold composite offers new implant options for bone repairs requiring immediate load bearing capacity.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12023" xmlns="http://purl.org/rss/1.0/"><title>Fabrication of Embedded Microstructures Via Lamination of Thick Gel-Casted Ceramic Layers</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12023</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Fabrication of Embedded Microstructures Via Lamination of Thick Gel-Casted Ceramic Layers</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Kean How Cheah, Jit Kai Chin</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-18T11:26:19.383153-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12023</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12023</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12023</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>This article describes a new approach to fabricate various embedded ceramic microstructures. Design geometries of the microstructures are replicated onto a soft reusable polydimethylsiloxane (PDMS) mold. Rapid consolidation of ceramic suspension on the molds using gel-casting technique produces structured ceramic layers. 85% aqueous glycerol solution has been identified as suitable adhesive agent to laminate the ceramic layers. Capability of the approach in fabricating embedded microstructures of 3-dimensional and aspect ratio as high as 20 and 50 has been demonstrated. Ceramic microthruster and Y-shaped microfluidic reactor are fabricated using this new approach to show its potential to construct various ceramic microdevices.</p></div>
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This article describes a new approach to fabricate various embedded ceramic microstructures. Design geometries of the microstructures are replicated onto a soft reusable polydimethylsiloxane (PDMS) mold. Rapid consolidation of ceramic suspension on the molds using gel-casting technique produces structured ceramic layers. 85% aqueous glycerol solution has been identified as suitable adhesive agent to laminate the ceramic layers. Capability of the approach in fabricating embedded microstructures of 3-dimensional and aspect ratio as high as 20 and 50 has been demonstrated. Ceramic microthruster and Y-shaped microfluidic reactor are fabricated using this new approach to show its potential to construct various ceramic microdevices.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12000" xmlns="http://purl.org/rss/1.0/"><title>Oxidation Behavior of Hot Pressed ZrB2-ZrC-SiC Ceramic Composites</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12000</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Oxidation Behavior of Hot Pressed ZrB2-ZrC-SiC Ceramic Composites</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yue Zhang, Dong Gao, Chunlai Xu, Yang Song, Xiaobin Shi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-11T11:32:19.315317-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12000</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12000</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12000</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Dense ZrB<sub>2</sub>-SiC ceramics containing 40 vol% ZrC particles are fabricated via hot pressing method. Then the sintered ceramics are oxidized in air up to 1500°C, and the oxidation kinetics of the ceramic composites is deduced in combination with the reacted fraction curves. As indicated by the experimental results, the oxidation kinetics changes from reaction-controlled process to diffusion-controlled one with increasing of oxidation temperature. In addition, the oxidation kinetics parameters are obtained, which indicates that the oxidation resistance decays at elevated temperatures. Furthermore, the evolution of surface morphology and oxide scale during oxidation process is clarified.</p></div>
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Dense ZrB2-SiC ceramics containing 40 vol% ZrC particles are fabricated via hot pressing method. Then the sintered ceramics are oxidized in air up to 1500°C, and the oxidation kinetics of the ceramic composites is deduced in combination with the reacted fraction curves. As indicated by the experimental results, the oxidation kinetics changes from reaction-controlled process to diffusion-controlled one with increasing of oxidation temperature. In addition, the oxidation kinetics parameters are obtained, which indicates that the oxidation resistance decays at elevated temperatures. Furthermore, the evolution of surface morphology and oxide scale during oxidation process is clarified.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12027" xmlns="http://purl.org/rss/1.0/"><title>Strength Behavior of Magnesia-Based Refractories after Thermal Cycling</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12027</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Strength Behavior of Magnesia-Based Refractories after Thermal Cycling</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Peter A. Olubambi, Anthony Andrews, Thabang S. Mothle</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-10T11:09:11.744842-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12027</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12027</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12027</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The thermal shock resistance of four commercially available magnesia-based refractory bricks mainly used in furnace linings were investigated. Thermal stability of the bricks was tested using the water-quench method. The experimental damage was characterised by visual inspection and determining some residual physical and mechanical properties. Cracks were observed after thermal cycling resulting in loss of strength and materials degradation. The results show that thermal stability of magnesia-based refractories depends strongly on their chemical composition. The addition of chrome and spinel improved the thermal stability of magnesia bricks with magnesia–spinel (MgAl<sub>2</sub>O<sub>4</sub>) having better thermal stability than the magnesia–chrome bricks.</p></div>
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The thermal shock resistance of four commercially available magnesia-based refractory bricks mainly used in furnace linings were investigated. Thermal stability of the bricks was tested using the water-quench method. The experimental damage was characterised by visual inspection and determining some residual physical and mechanical properties. Cracks were observed after thermal cycling resulting in loss of strength and materials degradation. The results show that thermal stability of magnesia-based refractories depends strongly on their chemical composition. The addition of chrome and spinel improved the thermal stability of magnesia bricks with magnesia–spinel (MgAl2O4) having better thermal stability than the magnesia–chrome bricks.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12026" xmlns="http://purl.org/rss/1.0/"><title>Effect of CaO Addition on Compressive Deformation of Silicon Nitride Ceramic with Y-Mg-Si-O-N Glassy System</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12026</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of CaO Addition on Compressive Deformation of Silicon Nitride Ceramic with Y-Mg-Si-O-N Glassy System</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Raayaa Wananuruksawong, Yutaka Shinoda, Takashi Akatsu, Fumihiro Wakai</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-10T11:09:07.431247-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12026</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12026</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12026</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Creep behavior of <span class="fixed-roman">Si<sub>3</sub>N<sub>4</sub></span> polycrystals containing <span class="fixed-roman">Y<sub>2</sub>O<sub>3</sub></span>-<span class="fixed-roman">MgO</span>-<span class="fixed-roman">SiO<sub>2</sub></span> glass phase (with and without Calcium oxide [<span class="fixed-roman">CaO</span>] additive) was studied by compression tests between 1500 and 1700°C. We studied the effect of <span class="fixed-roman">CaO</span> additive on flow stress, microstructural evolutions, and thermal stability of the intergranular glass phase during deformation. While the addition of <span class="fixed-roman">CaO</span> did not affect grain size, the flow stress decreased with the amount of CaO. This result suggested that the addition of <span class="fixed-roman">CaO</span> reduced the viscosity of intergranular glass phase. The addition of <span class="fixed-roman">CaO</span> further improved the thermal stability of the glass phase by suppressing the evaporation at elevated temperatures.</p></div>
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Creep behavior of Si3N4 polycrystals containing Y2O3-MgO-SiO2 glass phase (with and without Calcium oxide [CaO] additive) was studied by compression tests between 1500 and 1700°C. We studied the effect of CaO additive on flow stress, microstructural evolutions, and thermal stability of the intergranular glass phase during deformation. While the addition of CaO did not affect grain size, the flow stress decreased with the amount of CaO. This result suggested that the addition of CaO reduced the viscosity of intergranular glass phase. The addition of CaO further improved the thermal stability of the glass phase by suppressing the evaporation at elevated temperatures.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12025" xmlns="http://purl.org/rss/1.0/"><title>Shear Strength Measurement of AV119 Epoxy-Joined SiC by Different Torsion Tests</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12025</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Shear Strength Measurement of AV119 Epoxy-Joined SiC by Different Torsion Tests</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Monica Ferraris, Andrea Ventrella, Milena Salvo, Dietmar Gross</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-10T11:07:15.796398-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12025</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12025</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12025</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The results of an experimental investigation on epoxy-joined silicon carbide tested in shear mode by seven different configurations of torsion tests are presented and compared to results obtained by asymmetric four-point bending. All samples have been joined by an epoxy adhesive (Araldite AV119) chosen to obtain several joined samples in a reasonable time. Advantages and disadvantages of each configuration are discussed with the aim of finding a suitable method to measure the shear strength of joined components.</p></div>
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The results of an experimental investigation on epoxy-joined silicon carbide tested in shear mode by seven different configurations of torsion tests are presented and compared to results obtained by asymmetric four-point bending. All samples have been joined by an epoxy adhesive (Araldite AV119) chosen to obtain several joined samples in a reasonable time. Advantages and disadvantages of each configuration are discussed with the aim of finding a suitable method to measure the shear strength of joined components.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12028" xmlns="http://purl.org/rss/1.0/"><title>Complex Permittivity and Microwave-Absorbing Properties of Fe/Al2O3 Coatings by Air Plasma Spraying Technique</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12028</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Complex Permittivity and Microwave-Absorbing Properties of Fe/Al2O3 Coatings by Air Plasma Spraying Technique</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dong Zhao, Fa Luo, Wancheng Zhou, Dongmei Zhu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-10T10:56:02.942305-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12028</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12028</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12028</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The Fe/Al<sub>2</sub>O<sub>3</sub> coatings for application as microwave absorbers were deposited by air plasma spraying (APS). The morphologies of powders and cross-section of coatings were characterized by scanning electron microscope (SEM). The investigations of electrical conductivity and complex permittivity properties of coatings were performed. The real part (ε′) of permittivity increases with increasing Fe volume fraction, which is attributed to the space charge polarization, and the imaginary part (ε″) also increases which is ascribed to the increasing electrical conductivity result from the formation of Fe conductive network. The effect of Fe content on dielectric properties and the corresponding mechanisms are analyzed. By measuring the microwave absorption properties of the Fe/Al<sub>2</sub>O<sub>3</sub> coatings as a single-layer absorbers, it was find that the reflection loss varies with the changes of thickness and Fe content, due to the deviation of impedance-matching condition.</p></div>
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The Fe/Al2O3 coatings for application as microwave absorbers were deposited by air plasma spraying (APS). The morphologies of powders and cross-section of coatings were characterized by scanning electron microscope (SEM). The investigations of electrical conductivity and complex permittivity properties of coatings were performed. The real part (ε′) of permittivity increases with increasing Fe volume fraction, which is attributed to the space charge polarization, and the imaginary part (ε″) also increases which is ascribed to the increasing electrical conductivity result from the formation of Fe conductive network. The effect of Fe content on dielectric properties and the corresponding mechanisms are analyzed. By measuring the microwave absorption properties of the Fe/Al2O3 coatings as a single-layer absorbers, it was find that the reflection loss varies with the changes of thickness and Fe content, due to the deviation of impedance-matching condition.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12002" xmlns="http://purl.org/rss/1.0/"><title>Self-Healing Behavior of Barium–Lanthanum–Borosilicate Glass and Its Reactivity with Different Electrolytes for SOFC Applications</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12002</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Self-Healing Behavior of Barium–Lanthanum–Borosilicate Glass and Its Reactivity with Different Electrolytes for SOFC Applications</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Gurbinder Kaur, Om P. Pandey, Kulvir Singh</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-11-12T12:29:52.708989-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12002</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12002</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12002</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The diffusion couples of lanthanum-based barium borosilicate glass with high- and low-temperature electrolytes have been heat-treated at 850°C and 800°C, respectively, for 5, 100 and 750 h. These prepared diffusion couples have been characterized using various techniques like X-ray diffraction (XRD), scanning electron microscopy (SEM), X-ray dot mapping, and electron probe microanalysis (EPMA). The thermodynamic parameters like frequency factor, crystallization constants, free volume, and bulk thermal expansion coefficients have been calculated to understand the behavior of glass. Interestingly, glass revealed self-healing tendency with heat treatment duration.</p></div>
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The diffusion couples of lanthanum-based barium borosilicate glass with high- and low-temperature electrolytes have been heat-treated at 850°C and 800°C, respectively, for 5, 100 and 750 h. These prepared diffusion couples have been characterized using various techniques like X-ray diffraction (XRD), scanning electron microscopy (SEM), X-ray dot mapping, and electron probe microanalysis (EPMA). The thermodynamic parameters like frequency factor, crystallization constants, free volume, and bulk thermal expansion coefficients have been calculated to understand the behavior of glass. Interestingly, glass revealed self-healing tendency with heat treatment duration.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12004" xmlns="http://purl.org/rss/1.0/"><title>Prevention of Cracks in Functionally Graded SiO2-Mo Materials Fabricated by Uniaxial Compression Casting and Pressureless Sintering</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12004</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Prevention of Cracks in Functionally Graded SiO2-Mo Materials Fabricated by Uniaxial Compression Casting and Pressureless Sintering</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Takuya Honma, Ikue Sasaki, Nobuhiro Tamura, Junichi Tatami, Shinichiro Fujichika, Katsutoshi Komeya, Takeshi Meguro</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-11-08T09:25:44.913892-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12004</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12004</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12004</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>In industrial high-intensity discharge lamps, cracks and delaminations occasionally develop at the interface between <span class="fixed-roman">SiO<sub>2</sub></span> and the <span class="fixed-roman">Mo</span> foil in the seal. Here, functionally graded <span class="fixed-roman">SiO<sub>2</sub>-Mo</span> materials for use in these lamps were fabricated by uniaxial compression casting and pressureless sintering. Consequently, vertical cracks developed across the sintered body layers, and interfacial cracks developed between the 100 wt% <span class="fixed-roman">SiO<sub>2</sub></span> and 90 wt% <span class="fixed-roman">SiO<sub>2</sub>-Mo</span> layers. Therefore, the effects of residual stress, difference in the coefficient of thermal expansion (CTE), and difference in the volume shrinkage on these cracks were investigated. Vertical cracks were suppressed when residual stress was relaxed by annealing near the annealing point of silica glass during the cooling step in the sintering process. Interfacial cracks were suppressed when the difference in the CTE of the interface between the 100 wt% <span class="fixed-roman">SiO<sub>2</sub></span> and 90 wt% <span class="fixed-roman">SiO<sub>2</sub>-Mo</span> layers was relaxed by inserting layers of 95 wt% <span class="fixed-roman">SiO<sub>2</sub>-Mo</span> between them. Furthermore, the suppression effect became stronger when the difference in the volume shrinkage of the layers was relaxed by sintering to join the separately sintered monolayers. Thus, the development of these cracks was influenced by the residual stress, CTE, and volume shrinkage. Therefore, these cracks can be prevented by optimizing these factors.</p></div>
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In industrial high-intensity discharge lamps, cracks and delaminations occasionally develop at the interface between SiO2 and the Mo foil in the seal. Here, functionally graded SiO2-Mo materials for use in these lamps were fabricated by uniaxial compression casting and pressureless sintering. Consequently, vertical cracks developed across the sintered body layers, and interfacial cracks developed between the 100 wt% SiO2 and 90 wt% SiO2-Mo layers. Therefore, the effects of residual stress, difference in the coefficient of thermal expansion (CTE), and difference in the volume shrinkage on these cracks were investigated. Vertical cracks were suppressed when residual stress was relaxed by annealing near the annealing point of silica glass during the cooling step in the sintering process. Interfacial cracks were suppressed when the difference in the CTE of the interface between the 100 wt% SiO2 and 90 wt% SiO2-Mo layers was relaxed by inserting layers of 95 wt% SiO2-Mo between them. Furthermore, the suppression effect became stronger when the difference in the volume shrinkage of the layers was relaxed by sintering to join the separately sintered monolayers. Thus, the development of these cracks was influenced by the residual stress, CTE, and volume shrinkage. Therefore, these cracks can be prevented by optimizing these factors.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12003" xmlns="http://purl.org/rss/1.0/"><title>Effects of ZnO and B2O3 on the Microstructure and Microwave Dielectric Properties of 5Li2O-1Nb2O5-5TiO2 Ceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12003</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effects of ZnO and B2O3 on the Microstructure and Microwave Dielectric Properties of 5Li2O-1Nb2O5-5TiO2 Ceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Qun Zeng,, Nana Zhang, Yongheng Zhou, Weichao Zhan, Xiaoting Hong</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-11-08T09:25:42.569609-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12003</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12003</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12003</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The effects of ZnO and B<sub>2</sub>O<sub>3</sub> addition on the sintering behavior, microstructure, and the microwave dielectric properties of 5Li<sub>2</sub>O-1Nb<sub>2</sub>O<sub>5</sub>-5TiO<sub>2</sub> (LNT) ceramics have been investigated. With addition of low-level doping of ZnO and B<sub>2</sub>O<sub>3</sub>, the sintering temperature of the LNT ceramics can be lowered down to near 920°C due to the liquid phase effect. The Li<sub>2</sub>TiO<sub>3</sub>ss and the “M-phase” are the two main phases, whereas other phase could be observed when co-doping with ZnO and B<sub>2</sub>O<sub>3</sub> in the ceramics. And the amount of the other phase increases with the ZnO content increasing. The addition of ZnO does not induce much degradation in the microwave dielectric properties but lowers the τ<sub><em>f</em></sub> value to near zero. Typically, the good microwave dielectric properties of ε<sub><em>r</em></sub> = 36.4, <em>Q</em> × <em>f </em>=<em> </em>8835 GHz, τ<sub><em>f</em></sub> = 4.4 ppm/°C could be obtained for the 1 wt% B<sub>2</sub>O<sub>3</sub> and 4 wt% ZnO co-doped sample sintered at 920°C, which is promising for application of the multilayer microwave devices using Ag as internal electrode.</p></div>
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The effects of ZnO and B2O3 addition on the sintering behavior, microstructure, and the microwave dielectric properties of 5Li2O-1Nb2O5-5TiO2 (LNT) ceramics have been investigated. With addition of low-level doping of ZnO and B2O3, the sintering temperature of the LNT ceramics can be lowered down to near 920°C due to the liquid phase effect. The Li2TiO3ss and the “M-phase” are the two main phases, whereas other phase could be observed when co-doping with ZnO and B2O3 in the ceramics. And the amount of the other phase increases with the ZnO content increasing. The addition of ZnO does not induce much degradation in the microwave dielectric properties but lowers the τf value to near zero. Typically, the good microwave dielectric properties of εr = 36.4, Q × f = 8835 GHz, τf = 4.4 ppm/°C could be obtained for the 1 wt% B2O3 and 4 wt% ZnO co-doped sample sintered at 920°C, which is promising for application of the multilayer microwave devices using Ag as internal electrode.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02856.x" xmlns="http://purl.org/rss/1.0/"><title>Synthesis of Nanosized Cesium Ferrite by Precursor and Combustion Method: A Comparative Study</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02856.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Synthesis of Nanosized Cesium Ferrite by Precursor and Combustion Method: A Comparative Study</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Manik Gupta, Munish Gupta, Balwinder S. Randhawa</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-10-25T11:20:54.773484-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02856.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02856.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02856.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Topical Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Thermolysis of cesium hexa(carboxylato)ferrate(III) precursors, <span class="fixed-roman">Cs<sub>3</sub>[Fe(L)<sub>6</sub>].xH<sub>2</sub>O</span> (L = formate, acetate, propionate, butyrate), has been carried out in flowing air atmosphere from ambient temperature to 1000°C. Various physico-chemical techniques, that is, simultaneous TG-DTG-DTA, XRD, TEM, IR, Mössbauer spectroscopy, have been employed to characterize the intermediates and end products. After dehydration, the anhydrous precursors undergo exothermic decomposition to yield various intermediates, that is, cesium carbonate/propionate/butyrate and α-<span class="fixed-roman">Fe<sub>2</sub>O<sub>3</sub></span>. A subsequent decomposition of these intermediates leads to the formation of cesium ferrite above 800°C. Similar ferrite has been prepared by the combustion method at comparatively lower temperature (600°C) and in less time than that of conventional ceramic method.</p></div>
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Thermolysis of cesium hexa(carboxylato)ferrate(III) precursors, Cs3[Fe(L)6].xH2O (L = formate, acetate, propionate, butyrate), has been carried out in flowing air atmosphere from ambient temperature to 1000°C. Various physico-chemical techniques, that is, simultaneous TG-DTG-DTA, XRD, TEM, IR, Mössbauer spectroscopy, have been employed to characterize the intermediates and end products. After dehydration, the anhydrous precursors undergo exothermic decomposition to yield various intermediates, that is, cesium carbonate/propionate/butyrate and α-Fe2O3. A subsequent decomposition of these intermediates leads to the formation of cesium ferrite above 800°C. Similar ferrite has been prepared by the combustion method at comparatively lower temperature (600°C) and in less time than that of conventional ceramic method.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02855.x" xmlns="http://purl.org/rss/1.0/"><title>Preparation and Characterization of CIGSe Solar Cells by Ink Printing on Alumina Substrates with Self-Synthesized Selenide Powders via an Environment-Friendly and Cost-Effective Dry Synthesis Route</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02855.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Preparation and Characterization of CIGSe Solar Cells by Ink Printing on Alumina Substrates with Self-Synthesized Selenide Powders via an Environment-Friendly and Cost-Effective Dry Synthesis Route</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dong-Hau Kuo, Cian-Wei Jhang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-10-25T11:20:26.932587-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02855.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02855.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02855.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>CIGSe solar cells with an ink-printing absorber layer were prepared on Mo-coated alumina substrates. The use of alumina substrates can extend the process window to higher temperatures. The inks contained single-phase CIGSe powder, which was formed by firing different selenide powders of Cu<sub>2</sub>Se, In<sub>2</sub>Se<sub>3</sub>, and Ga<sub>2</sub>Se<sub>3</sub> at 800°C. All these powders were synthesized with an environment-friendly and cost-effective powder process. The printed inks were sintered at 600–800°C. The solar cells had power conversion efficiency of 0.50%, an open-circuit voltage of 27 mV, a short-circuit current density of 37 mA/cm<sup>2</sup>, and a fill factor of 0.50.</p></div>
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CIGSe solar cells with an ink-printing absorber layer were prepared on Mo-coated alumina substrates. The use of alumina substrates can extend the process window to higher temperatures. The inks contained single-phase CIGSe powder, which was formed by firing different selenide powders of Cu2Se, In2Se3, and Ga2Se3 at 800°C. All these powders were synthesized with an environment-friendly and cost-effective powder process. The printed inks were sintered at 600–800°C. The solar cells had power conversion efficiency of 0.50%, an open-circuit voltage of 27 mV, a short-circuit current density of 37 mA/cm2, and a fill factor of 0.50.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02853.x" xmlns="http://purl.org/rss/1.0/"><title>Joining of Silicon Nitride by Local Heating for Fabrication of Long Ceramic Pipes</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02853.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Joining of Silicon Nitride by Local Heating for Fabrication of Long Ceramic Pipes</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mikinori Hotta, Naoki Kondo, Hideki Kita, Tatsuki Ohji, Yasuhisa Izutsu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-10-25T11:19:53.299809-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02853.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02853.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02853.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>This study demonstrated that a long silicon nitride pipe of several meters with adequately strong joints can be fabricated by a local-heating joining technique. Commercially available silicon nitride ceramic pipes sintered with Y<sub>2</sub>O<sub>3</sub> and Al<sub>2</sub>O<sub>3</sub> additives were used for parent material, and powder slurry of Si<sub>3</sub>N<sub>4</sub>-Y<sub>2</sub>O<sub>3</sub>-Al<sub>2</sub>O<sub>3</sub>-SiO<sub>2</sub> system was brush-coated on the rough or uneven end faces of the pipes. Joining was carried out by locally heating the joint region at different temperatures from 1500°C to 1650°C for 1 h with a mechanical pressure of 5 MPa in N<sub>2</sub> flow; using a horizontal electrical furnace specially designed for this experiment. The silicon nitride pipe 3-m long was successfully fabricated without voids or cracks in the joint region, and the microstructure of the joint region was similar to that of the parent one. The joint strength was examined in flexure using specimens cut from the joined pipes, and those joined at 1600°C and 1650°C indicated the highest strength of about 680 MPa, which was almost the same as that of the parent material. This study also indicated that the slurry brush-coating technique is advantageous to easily joining ceramic pipes with rough or uneven end faces, which is essentially important for practical use.</p></div>
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This study demonstrated that a long silicon nitride pipe of several meters with adequately strong joints can be fabricated by a local-heating joining technique. Commercially available silicon nitride ceramic pipes sintered with Y2O3 and Al2O3 additives were used for parent material, and powder slurry of Si3N4-Y2O3-Al2O3-SiO2 system was brush-coated on the rough or uneven end faces of the pipes. Joining was carried out by locally heating the joint region at different temperatures from 1500°C to 1650°C for 1 h with a mechanical pressure of 5 MPa in N2 flow; using a horizontal electrical furnace specially designed for this experiment. The silicon nitride pipe 3-m long was successfully fabricated without voids or cracks in the joint region, and the microstructure of the joint region was similar to that of the parent one. The joint strength was examined in flexure using specimens cut from the joined pipes, and those joined at 1600°C and 1650°C indicated the highest strength of about 680 MPa, which was almost the same as that of the parent material. This study also indicated that the slurry brush-coating technique is advantageous to easily joining ceramic pipes with rough or uneven end faces, which is essentially important for practical use.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02852.x" xmlns="http://purl.org/rss/1.0/"><title>Colloidal Shaping of 8 mol% Yttria-Stabilized Zirconia Electrolyte Honeycomb Structures by Microwave-Assisted Thermal Gelation of Methyl Cellulose</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02852.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Colloidal Shaping of 8 mol% Yttria-Stabilized Zirconia Electrolyte Honeycomb Structures by Microwave-Assisted Thermal Gelation of Methyl Cellulose</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Kotikalapudi Rajeswari, Papiya Biswas, Madireddy Buchi Suresh, Unnikrishnan Saraswathy Hareesh, Roy Johnson, Dibakar Das</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-10-25T11:19:38.652452-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02852.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02852.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02852.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Eight mol% Yttria-stabilized zirconia, the most commonly employed electrolyte material for solid oxide fuel cells (SOFC), was shaped into honeycomb structures by thermally induced gelation of aqueous zirconia slurry containing methyl cellulose using microwave irradiation. The green honeycomb samples were subjected to green density and green compressive strength measurements revealing a uniform gelation and hence a relatively higher strength for microwave irradiated samples. The green honeycomb samples were further sintered to crack-free dense honeycombs (&gt;99% TD) at 1525°C for 1 h. Honeycomb samples were characterized for their physical, cellular, and electrical properties. A relatively high ionic conductivity value of 0.07 S/cm at 800°C and corresponding low activation energy of 0.61 eV in the temperature range 700–800°C provide opportunities to explore the development of novel designs for SOFC application.</p></div>
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Eight mol% Yttria-stabilized zirconia, the most commonly employed electrolyte material for solid oxide fuel cells (SOFC), was shaped into honeycomb structures by thermally induced gelation of aqueous zirconia slurry containing methyl cellulose using microwave irradiation. The green honeycomb samples were subjected to green density and green compressive strength measurements revealing a uniform gelation and hence a relatively higher strength for microwave irradiated samples. The green honeycomb samples were further sintered to crack-free dense honeycombs (&gt;99% TD) at 1525°C for 1 h. Honeycomb samples were characterized for their physical, cellular, and electrical properties. A relatively high ionic conductivity value of 0.07 S/cm at 800°C and corresponding low activation energy of 0.61 eV in the temperature range 700–800°C provide opportunities to explore the development of novel designs for SOFC application.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02795.x" xmlns="http://purl.org/rss/1.0/"><title>Growth and Application of ZnO Nanostructures</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02795.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Growth and Application of ZnO Nanostructures</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">D. R. Sahu, Chuan-Pu Liu, Ruey-Chi Wang, Chien-Lin Kuo, Jow-Lay Huang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-10-18T10:43:41.294003-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02795.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02795.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02795.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Topical Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Nanostructures are the building blocks of future nanodevices and thus methods for fabricating nanostructures of various materials in various forms are fundamentally important. Among those nanostructures <span class="fixed-roman">ZnO</span> has received much attention over the past few years due to the wide range of research by many different groups focused on different novel nanostructures with different properties. Although <span class="fixed-roman">ZnO</span> nanowires have been intensively studied, there are only a few methods that showed promising characteristics for practical applications. Without much effort, it can be grown in many different nanostructure forms, thus allowing various novel devices to be achieved. In this study, we intend to review those methods that enable nanostructure growth to be more controllable and feasible for applications. The methods for fabricating <span class="fixed-roman">ZnO</span> nanostructures are introduced in the first part. In the second part, the application of those nanostructures are mentioned and explained. Finally, the future realization of nanodevices is discussed.</p></div>
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Nanostructures are the building blocks of future nanodevices and thus methods for fabricating nanostructures of various materials in various forms are fundamentally important. Among those nanostructures ZnO has received much attention over the past few years due to the wide range of research by many different groups focused on different novel nanostructures with different properties. Although ZnO nanowires have been intensively studied, there are only a few methods that showed promising characteristics for practical applications. Without much effort, it can be grown in many different nanostructure forms, thus allowing various novel devices to be achieved. In this study, we intend to review those methods that enable nanostructure growth to be more controllable and feasible for applications. The methods for fabricating ZnO nanostructures are introduced in the first part. In the second part, the application of those nanostructures are mentioned and explained. Finally, the future realization of nanodevices is discussed.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02848.x" xmlns="http://purl.org/rss/1.0/"><title>Materials Challenges in Reverse-Flow Pyrolysis Reactors for Petrochemical Applications</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02848.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Materials Challenges in Reverse-Flow Pyrolysis Reactors for Petrochemical Applications</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Chang Min Chun, Sanket Desai, Frank Hershkowitz, Paul F. Keusenkothen, Gary D. Mohr, Trikur A. Ramanarayanan</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-10-15T16:33:13.457848-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02848.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02848.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02848.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Currently, the pyrolysis of hydrocarbons for the production of light olefins is almost exclusively carried out in steam crackers operating around 900–1000°C. However, cracking hydrocarbons at much higher temperature results in high selectivity to acetylene, which can be converted into many petrochemical products including ethylene. The desired hydropyrolysis reaction from hydrocarbons to acetylene can be realized in a reverse-flow reactor at very high temperatures (&gt;1700°C) in a scalable manner. The reactor elements include ceramic components that are placed in the hottest regions of the reactor and must withstand a temperature that is in the range of 1500–2000°C. In addition, the temperature rises and falls with the reverse-flow cycle; a fluctuation that could be as high as 100–500°C over a period of several seconds. Moreover, the materials in the hot zone are exposed alternately to a regeneration (heat addition) step that is mildly oxidizing, and a pyrolysis (cracking) step that is strongly reducing with a correspondingly high carbon activity. This article addresses the thermodynamic stability of selected ceramic materials based on alumina, zirconia, and yttria for such an application. Results from laboratory tests involving the exposure of these ceramic materials to simulated process conditions followed by their microstructural characterization are compared with expectations from thermodynamic predictions.</p></div>
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Currently, the pyrolysis of hydrocarbons for the production of light olefins is almost exclusively carried out in steam crackers operating around 900–1000°C. However, cracking hydrocarbons at much higher temperature results in high selectivity to acetylene, which can be converted into many petrochemical products including ethylene. The desired hydropyrolysis reaction from hydrocarbons to acetylene can be realized in a reverse-flow reactor at very high temperatures (&gt;1700°C) in a scalable manner. The reactor elements include ceramic components that are placed in the hottest regions of the reactor and must withstand a temperature that is in the range of 1500–2000°C. In addition, the temperature rises and falls with the reverse-flow cycle; a fluctuation that could be as high as 100–500°C over a period of several seconds. Moreover, the materials in the hot zone are exposed alternately to a regeneration (heat addition) step that is mildly oxidizing, and a pyrolysis (cracking) step that is strongly reducing with a correspondingly high carbon activity. This article addresses the thermodynamic stability of selected ceramic materials based on alumina, zirconia, and yttria for such an application. Results from laboratory tests involving the exposure of these ceramic materials to simulated process conditions followed by their microstructural characterization are compared with expectations from thermodynamic predictions.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02851.x" xmlns="http://purl.org/rss/1.0/"><title>Effect of Calcinating Temperature and Mn doping on Dielectric Properties of temperature-stable BaTiO3-Based X8R Ceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02851.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of Calcinating Temperature and Mn doping on Dielectric Properties of temperature-stable BaTiO3-Based X8R Ceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Baolin Zhang, Shunhua Wu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-10-11T10:37:53.443879-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02851.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02851.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02851.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Systematic investigation has been made on the structure and dielectric properties of MnCO<sub>3</sub>-doped barium titanate-based X8R ceramics, to reveal the relationship between the manufacturing process and dielectric properties. The dielectric ceramic sintered at 950°C showed high permittivity and low dielectric loss, meeting X8R specifications. Transmission electron microscopy and EDS analysis were used. The results suggested that the temperature-stable BaTiO<sub>3</sub>-based X8R ceramics with the good dielectric properties can be prepared through the BaTiO<sub>3</sub> calcined at 1150°C and doped with 0.7 wt% MnCO<sub>3.</sub></p></div>
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Systematic investigation has been made on the structure and dielectric properties of MnCO3-doped barium titanate-based X8R ceramics, to reveal the relationship between the manufacturing process and dielectric properties. The dielectric ceramic sintered at 950°C showed high permittivity and low dielectric loss, meeting X8R specifications. Transmission electron microscopy and EDS analysis were used. The results suggested that the temperature-stable BaTiO3-based X8R ceramics with the good dielectric properties can be prepared through the BaTiO3 calcined at 1150°C and doped with 0.7 wt% MnCO3.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02850.x" xmlns="http://purl.org/rss/1.0/"><title>Ceramic Coatings and Glass Additives for Improved SiC-Based Filters for Molten Iron Filtration</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02850.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Ceramic Coatings and Glass Additives for Improved SiC-Based Filters for Molten Iron Filtration</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Michael C. Tucker, Jay Tu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-10-11T10:37:15.367981-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02850.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02850.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02850.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Reticulated silicon carbide (SiC) ceramic filters are prepared with modified coatings in an attempt to improve mechanical properties of the sintered filter. Two classes of coatings are used: mixtures of non-SiC ceramic and sintering aid and mixtures of SiC and glass. Various candidate ceramics, sintering aids, and glasses are screened. The most promising coatings are determined to be silica with 5 wt% bismuth oxide and SiC with ≤10 wt% Spruce Pine Batch glass. Filters with these coatings are prepared and subjected to mechanical abuse. Both coatings improve the ruggedness of the filter relative to the standard uncoated SiC type. Filters with &lt;10 wt% glass additive were subjected to molten metal impingement and filtration of liquid gray iron at 1510°C. Those with 5 wt% glass or more softened during filtration. Those with 2.5 wt% glass or less survived without failure.</p></div>
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Reticulated silicon carbide (SiC) ceramic filters are prepared with modified coatings in an attempt to improve mechanical properties of the sintered filter. Two classes of coatings are used: mixtures of non-SiC ceramic and sintering aid and mixtures of SiC and glass. Various candidate ceramics, sintering aids, and glasses are screened. The most promising coatings are determined to be silica with 5 wt% bismuth oxide and SiC with ≤10 wt% Spruce Pine Batch glass. Filters with these coatings are prepared and subjected to mechanical abuse. Both coatings improve the ruggedness of the filter relative to the standard uncoated SiC type. Filters with &lt;10 wt% glass additive were subjected to molten metal impingement and filtration of liquid gray iron at 1510°C. Those with 5 wt% glass or more softened during filtration. Those with 2.5 wt% glass or less survived without failure.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02849.x" xmlns="http://purl.org/rss/1.0/"><title>The Effect of Grain Size on the Mechanical and Optical Properties of Spark Plasma Sintering-Processed Magnesium Aluminate Spinel MgAl2O4</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02849.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">The Effect of Grain Size on the Mechanical and Optical Properties of Spark Plasma Sintering-Processed Magnesium Aluminate Spinel MgAl2O4</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Amnon Rothman, Sergey Kalabukhov, Nataliya Sverdlov, Moshe P. Dariel, Nahum Frage</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-10-11T10:37:12.62837-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02849.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02849.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02849.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The study deals with the effect of the SPS parameters and LiF doping on the mechanical and optical properties polycrystalline magnesium aluminate spinel (PMAS) with emphasis on the grain size of the final product. Sintering at 1300°C of undoped powder yielded fully dense submicrometer (0.4–0.6 μm) samples with elevated mechanical properties (1600HV and 300MPa bending strength). Doped samples had a larger, 40 μm grain size, lower, 1450HV, hardness and 150MPa bending strength. The transmittance of the doped samples (80% at 500 nm wavelength) was higher than that of the undoped ones. Thus, the required functionality of the ceramic dictates the choice of parameters for the fabrication of dense transparent PMAS.</p></div>
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The study deals with the effect of the SPS parameters and LiF doping on the mechanical and optical properties polycrystalline magnesium aluminate spinel (PMAS) with emphasis on the grain size of the final product. Sintering at 1300°C of undoped powder yielded fully dense submicrometer (0.4–0.6 μm) samples with elevated mechanical properties (1600HV and 300MPa bending strength). Doped samples had a larger, 40 μm grain size, lower, 1450HV, hardness and 150MPa bending strength. The transmittance of the doped samples (80% at 500 nm wavelength) was higher than that of the undoped ones. Thus, the required functionality of the ceramic dictates the choice of parameters for the fabrication of dense transparent PMAS.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02839.x" xmlns="http://purl.org/rss/1.0/"><title>Tape Casting of Anode Supports for Solid Oxide Fuel Cells at Forschungszentrum Jülich</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02839.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Tape Casting of Anode Supports for Solid Oxide Fuel Cells at Forschungszentrum Jülich</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Wolfgang Schafbauer, Norbert H. Menzler,, Hans P. Buchkremer</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-10-04T11:05:39.843772-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02839.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02839.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02839.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>This contribution describes the development of tape casting for solid oxide fuel cells (SOFCs) anode supports starting with the characterization of the powders and ending with manufacturing of cells for stack testing. After casting the support, full cells were prepared by screen printing and sintering of the functional layers. The results of single-cell and stack tests of the novel SOFC will be discussed. The new cell showed excellent electrochemical performance in single-cell tests with more than 1.5 A/cm<sup>2</sup> (800°C, 0.7 V). Furthermore, stack tests showed no significant difference from earlier standard cells when operated at 800°C with a current density of 0.5 A/cm<sup>2</sup>.</p></div>
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This contribution describes the development of tape casting for solid oxide fuel cells (SOFCs) anode supports starting with the characterization of the powders and ending with manufacturing of cells for stack testing. After casting the support, full cells were prepared by screen printing and sintering of the functional layers. The results of single-cell and stack tests of the novel SOFC will be discussed. The new cell showed excellent electrochemical performance in single-cell tests with more than 1.5 A/cm2 (800°C, 0.7 V). Furthermore, stack tests showed no significant difference from earlier standard cells when operated at 800°C with a current density of 0.5 A/cm2.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02842.x" xmlns="http://purl.org/rss/1.0/"><title>High-Temperature Shear Strength and Bonding Mechanism of the Mullite Ceramic/Fiber Brick Component Joined by Phosphate Adhesive</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02842.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">High-Temperature Shear Strength and Bonding Mechanism of the Mullite Ceramic/Fiber Brick Component Joined by Phosphate Adhesive</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ruihua Hao, Jiachen Liu, Xue Dong, Anran Guo, Zhenguang Hou, Min Wang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-10-04T11:05:35.872481-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02842.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02842.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02842.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The mullite ceramic/fiber brick system was bonded by two kinds of phosphate adhesives. The specimens were treated from 200 to 1400°C. The mechanical properties were tested at room temperature and at high temperature, and the relevant bonding mechanism was also discussed. The results show that the addition of silicon can greatly improve the adhesive's mechanical properties. The room-temperature shear strength of the component bonded by adhesive with the silicon calcined at 800°C can reach 6.58 MPa. The shear strength of the adhesive with silicon tested at 800°C can reach 0.42 MPa.</p></div>
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The mullite ceramic/fiber brick system was bonded by two kinds of phosphate adhesives. The specimens were treated from 200 to 1400°C. The mechanical properties were tested at room temperature and at high temperature, and the relevant bonding mechanism was also discussed. The results show that the addition of silicon can greatly improve the adhesive's mechanical properties. The room-temperature shear strength of the component bonded by adhesive with the silicon calcined at 800°C can reach 6.58 MPa. The shear strength of the adhesive with silicon tested at 800°C can reach 0.42 MPa.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02835.x" xmlns="http://purl.org/rss/1.0/"><title>Influence of B2O3 Additive on Microwave Dielectric Properties of Li2ZnTi3O8 Ceramics for LTCC Applications</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02835.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Influence of B2O3 Additive on Microwave Dielectric Properties of Li2ZnTi3O8 Ceramics for LTCC Applications</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Chih-Yi Liu, Bing-Guang Tsai, Min-Hang Weng, Shyh-Jer Huang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-10-04T11:05:33.602674-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02835.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02835.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02835.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The effect of <span class="fixed-roman">B</span><sub>2</sub><span class="fixed-roman">O</span><sub>3</sub> addition on the microwave dielectric properties and microstructure of <span class="fixed-roman">Li</span><sub>2</sub><span class="fixed-roman">ZnTi</span><sub>3</sub><span class="fixed-roman">O</span><sub>8</sub> ceramics prepared using conventional solid-state reaction was investigated for low-temperature co-fired ceramic (LTCC) applications. X-ray diffraction and scanning electron microscopy were used to investigate the effect of <span class="fixed-roman">B</span><sub>2</sub><span class="fixed-roman">O</span><sub>3</sub> addition on the sintering process. The <span class="fixed-roman">Li</span><sub>2</sub><span class="fixed-roman">ZnTi</span><sub>3</sub><span class="fixed-roman">O</span><sub>8</sub> ceramic sintered at 875°C with 0.5 wt% <span class="fixed-roman">B</span><sub>2</sub><span class="fixed-roman">O</span><sub>3</sub> for 4 h showed good microwave dielectric properties including ε<sub><em>r</em></sub> = 25, <em>Q</em> × <em>f</em> = 50,917 GHz, and τ<sub><em>f</em></sub> = −17.8 ppm/°C. Silver was found to be unreactive toward the 0.5 wt% <span class="fixed-roman">B</span><sub>2</sub><span class="fixed-roman">O</span><sub>3</sub> doped <span class="fixed-roman">Li</span><sub>2</sub><span class="fixed-roman">ZnTi</span><sub>3</sub><span class="fixed-roman">O</span><sub>8</sub> ceramic under the above sintering conditions.</p></div>
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The effect of B2O3 addition on the microwave dielectric properties and microstructure of Li2ZnTi3O8 ceramics prepared using conventional solid-state reaction was investigated for low-temperature co-fired ceramic (LTCC) applications. X-ray diffraction and scanning electron microscopy were used to investigate the effect of B2O3 addition on the sintering process. The Li2ZnTi3O8 ceramic sintered at 875°C with 0.5 wt% B2O3 for 4 h showed good microwave dielectric properties including εr = 25, Q × f = 50,917 GHz, and τf = −17.8 ppm/°C. Silver was found to be unreactive toward the 0.5 wt% B2O3 doped Li2ZnTi3O8 ceramic under the above sintering conditions.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02834.x" xmlns="http://purl.org/rss/1.0/"><title>New Non Phyto- and Eco-Toxic Alumina-Stabilized Silver and Praseodymium Nanoparticles</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02834.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">New Non Phyto- and Eco-Toxic Alumina-Stabilized Silver and Praseodymium Nanoparticles</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Agnieszka Maria Jastrzębska, Ewa Karwowska, Agnieszka Tabernacka, Paulina Mosdorf, Paweł Polis, Patrycja Kurtycz, Andrzej Olszyna, Antoni Ryszard Kunicki</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-10-04T11:05:30.797864-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02834.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02834.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02834.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>In the present study, we examined how the active aluminum nano-oxide in the gamma form used as a neutral carrier for the nanoparticles of various metals (as <span class="fixed-roman">Ag</span>, <span class="fixed-roman">Pr</span>) affected their toxic behavior. Our experiments have shown that exposure to metal nanoparticles can be reduced by binding the nanoparticles to alumina nanoparticles and the aluminum nano-oxide is suitable to function as the nano-stabilizer for the <span class="fixed-roman">Ag</span> and <span class="fixed-roman">Pr</span> nanoparticles. We have managed to manufacture new alumina-stabilized silver and praseodymium nanoparticles using dry sol-gel method that are not phyto- and eco-toxic.</p></div>
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In the present study, we examined how the active aluminum nano-oxide in the gamma form used as a neutral carrier for the nanoparticles of various metals (as Ag, Pr) affected their toxic behavior. Our experiments have shown that exposure to metal nanoparticles can be reduced by binding the nanoparticles to alumina nanoparticles and the aluminum nano-oxide is suitable to function as the nano-stabilizer for the Ag and Pr nanoparticles. We have managed to manufacture new alumina-stabilized silver and praseodymium nanoparticles using dry sol-gel method that are not phyto- and eco-toxic.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02847.x" xmlns="http://purl.org/rss/1.0/"><title>Evaluation of Air Permeation Behavior of Porous SiC Ceramics Synthesized by Oxidation-Bonding Technique</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02847.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Evaluation of Air Permeation Behavior of Porous SiC Ceramics Synthesized by Oxidation-Bonding Technique</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Atanu Dey, Nijhuma Kayal, Omprakash Chakrabarti, Murilo D. M. Innocentini, Welton S. Chacon, José R. Coury</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-10-03T14:45:27.074636-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02847.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02847.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02847.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Porous SiC ceramics were synthesized by oxidation bonding of compacts of commercial α-SiC powder at 1300°C. Different volume fractions of petroleum coke powder were used for variation of porosity of ceramics from 36% to 56%. The material exhibited variations of pore size from 3 to 15 μm, flexural strength from 5.5 to 29.5 MPa, and elastic modulus from 3.3 to 27.6 GPa. Air permeation behavior was studied at 26–650°C. At room temperature Darcian (<em>k</em><sub>1</sub>) and non-Darcian (<em>k</em><sub>2</sub>) permeability parameters vary from 1.64 to 18.42 × 10<sup>−13</sup> m<sup>2</sup> and 0.58 to 2.95 × 10<sup>−7</sup> m, respectively. Temperature dependence of permeability was explained from structural changes occurring during test conditions.</p></div>
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Porous SiC ceramics were synthesized by oxidation bonding of compacts of commercial α-SiC powder at 1300°C. Different volume fractions of petroleum coke powder were used for variation of porosity of ceramics from 36% to 56%. The material exhibited variations of pore size from 3 to 15 μm, flexural strength from 5.5 to 29.5 MPa, and elastic modulus from 3.3 to 27.6 GPa. Air permeation behavior was studied at 26–650°C. At room temperature Darcian (k1) and non-Darcian (k2) permeability parameters vary from 1.64 to 18.42 × 10−13 m2 and 0.58 to 2.95 × 10−7 m, respectively. Temperature dependence of permeability was explained from structural changes occurring during test conditions.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02846.x" xmlns="http://purl.org/rss/1.0/"><title>Microwave Dielectric Properties of Fused Silica Prepared by Different Approaches</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02846.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Microwave Dielectric Properties of Fused Silica Prepared by Different Approaches</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Lei Li, Yong Fang, Qing Xiao, Yong Jun Wu, Nan Wang, Xiang Ming Chen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-10-03T14:45:22.119142-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02846.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02846.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02846.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="ijac02846-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p>Fused silica was prepared by different approaches, and the microwave dielectric properties were investigated. For the fused silica sintered at 1100°C by solid-state sintering, the dielectric constant (ε<sub><em>r</em></sub>) and <em>Qf</em> value increased with increasing the sintering time up to 5 h, while the temperature coefficient of resonant frequency (τ<sub><em>f</em></sub>) decreased. The optimal properties with low ε<sub><em>r</em></sub> of 3.72, high <em>Qf</em> value of 44,300 GHz, and low τ<sub><em>f</em></sub> of −14.4 ppm/°C were achieved when sintered at 1100°C for 5 h. The microwave dielectric properties could be further improved by other preparing approaches, as listed below: ε<sub><em>r</em></sub> = 3.90, <em>Qf</em> = 63,500 GHz, τ<sub><em>f</em></sub> = −5.7 ppm/°C for spark plasma sintering, and ε<sub><em>r</em></sub> = 3.83, <em>Qf</em> = 122,100 GHz, τ<sub><em>f</em></sub> = −8.3 ppm/°C for melting method. The results showed that fused silica was a good candidate as a microwave substrate material.</p></div></div>
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Fused silica was prepared by different approaches, and the microwave dielectric properties were investigated. For the fused silica sintered at 1100°C by solid-state sintering, the dielectric constant (εr) and Qf value increased with increasing the sintering time up to 5 h, while the temperature coefficient of resonant frequency (τf) decreased. The optimal properties with low εr of 3.72, high Qf value of 44,300 GHz, and low τf of −14.4 ppm/°C were achieved when sintered at 1100°C for 5 h. The microwave dielectric properties could be further improved by other preparing approaches, as listed below: εr = 3.90, Qf = 63,500 GHz, τf = −5.7 ppm/°C for spark plasma sintering, and εr = 3.83, Qf = 122,100 GHz, τf = −8.3 ppm/°C for melting method. The results showed that fused silica was a good candidate as a microwave substrate material.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02819.x" xmlns="http://purl.org/rss/1.0/"><title>Photoluminescence Investigations of the Near White Light Emitting Perovskite Ceramic SrZrO3:Dy3+ Prepared Via Gel-Combustion Route</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02819.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Photoluminescence Investigations of the Near White Light Emitting Perovskite Ceramic SrZrO3:Dy3+ Prepared Via Gel-Combustion Route</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Santosh K. Gupta, Manoj Mohapatra, Venkataraman Natarajan, Shrikant V. Godbole</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-09-20T10:02:11.509761-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02819.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02819.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02819.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Trivalent dysprosium-doped strontium zirconate perovskite (<span class="fixed-roman">SrZrO</span><sub>3</sub>) phosphors were prepared by gel-combustion synthesis using citric acid as fuel and ammonium nitrate as oxidizer. X-ray diffraction patterns confirmed the formation of orthorhombic phase of <span class="fixed-roman">SrZrO</span><sub>3</sub> with minor impurity, which completely disappears at high temperature. The morphological investigation was carried out using scanning electron microscopy (SEM). Photoluminescence studies showed that no emission from the host is observed, indicating the efficient energy transfer from the <span class="fixed-roman">ZrO</span><sub>3</sub><sup>2−</sup> group to <span class="fixed-roman">Dy</span><sup>3+</sup> ions. The emission line is purely because of f–f transitions of <span class="fixed-roman">Dy</span><sup>3+</sup>. Moreover, these phosphors predominantly exhibit near white light emission, when excited by 229 nm UV light due to strong <sup>4</sup>F<sub>9/2</sub>→<sup>6</sup>H<sub>13/2</sub> transition at 577 nm (yellow), strong <sup>4</sup>F<sub>9/2</sub>→<sup>6</sup>H<sub>15/2</sub> transition at 482 nm (blue), and weak <sup>4</sup>F<sub>9/2</sub>→<sup>6</sup>H<sub>9/2</sub> transition at 677 nm (red). Enhancement in emission intensity was observed with increase in the annealing temperature of the phosphor. The CIE chromaticity coordinates of the <span class="fixed-roman">SrZrO</span><sub>3</sub>:<span class="fixed-roman">Dy</span><sup>3+</sup> phosphors were observed to fall in the white light domain of the chromaticity diagram, which indicate that such fine tuning might be possible after varying the temperature of annealing.</p></div>
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Trivalent dysprosium-doped strontium zirconate perovskite (SrZrO3) phosphors were prepared by gel-combustion synthesis using citric acid as fuel and ammonium nitrate as oxidizer. X-ray diffraction patterns confirmed the formation of orthorhombic phase of SrZrO3 with minor impurity, which completely disappears at high temperature. The morphological investigation was carried out using scanning electron microscopy (SEM). Photoluminescence studies showed that no emission from the host is observed, indicating the efficient energy transfer from the ZrO32− group to Dy3+ ions. The emission line is purely because of f–f transitions of Dy3+. Moreover, these phosphors predominantly exhibit near white light emission, when excited by 229 nm UV light due to strong 4F9/2→6H13/2 transition at 577 nm (yellow), strong 4F9/2→6H15/2 transition at 482 nm (blue), and weak 4F9/2→6H9/2 transition at 677 nm (red). Enhancement in emission intensity was observed with increase in the annealing temperature of the phosphor. The CIE chromaticity coordinates of the SrZrO3:Dy3+ phosphors were observed to fall in the white light domain of the chromaticity diagram, which indicate that such fine tuning might be possible after varying the temperature of annealing.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02822.x" xmlns="http://purl.org/rss/1.0/"><title>Study of Antibacterial Activity of Metal Nanoparticle Absorbed Fly-Ash based Ceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02822.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Study of Antibacterial Activity of Metal Nanoparticle Absorbed Fly-Ash based Ceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Parveen Sultana, Sukhen Das, Alakananda Bhattacharya, Ruma Basu, Papiya Nandy</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-09-20T10:02:07.924974-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02822.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02822.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02822.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The bactericidal action of silver nanoparticles has been observed by many researchers since few years. In this study, we have developed an antibacterial ceramics (ACs) by absorbing synthesized silver nanoparticles within the ceramic matrix developed by us from an abundantly available coal fly ash, an extremely hazardous by-product of thermal power plants. Nanoparticles dispersions of different particle sizes were made absorbed in to the ceramic matrix to evaluate its bactericidal activity against both <em>Staphylococcus aureus</em> (Gram-positive) and <em>Escherichia coli</em> (Gram-negative) bacteria, taken as the model microorganisms. This study showed that the total bactericidal action of ACs depends on the size of absorbed nanoparticles and the content of nanoparticles in the dispersions within the ceramic matrix. ACs thus developed release very slowly a minute amount of nanoparticles and show strong and prolonged bactericidal activity against pathogenic strain of both types of bacteria. The concentration of prepared nanoparticles in dispersion and the concentration of released nanoparticles in aqueous medium from the absorbed ceramic matrix were measured using inductively coupled plasma spectrophotometer. The mechanism of the antibacterial action was also studied using transmission electron microscopy image analysis of the bacterial cross-section of both types of bacteria.</p></div>
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The bactericidal action of silver nanoparticles has been observed by many researchers since few years. In this study, we have developed an antibacterial ceramics (ACs) by absorbing synthesized silver nanoparticles within the ceramic matrix developed by us from an abundantly available coal fly ash, an extremely hazardous by-product of thermal power plants. Nanoparticles dispersions of different particle sizes were made absorbed in to the ceramic matrix to evaluate its bactericidal activity against both Staphylococcus aureus (Gram-positive) and Escherichia coli (Gram-negative) bacteria, taken as the model microorganisms. This study showed that the total bactericidal action of ACs depends on the size of absorbed nanoparticles and the content of nanoparticles in the dispersions within the ceramic matrix. ACs thus developed release very slowly a minute amount of nanoparticles and show strong and prolonged bactericidal activity against pathogenic strain of both types of bacteria. The concentration of prepared nanoparticles in dispersion and the concentration of released nanoparticles in aqueous medium from the absorbed ceramic matrix were measured using inductively coupled plasma spectrophotometer. The mechanism of the antibacterial action was also studied using transmission electron microscopy image analysis of the bacterial cross-section of both types of bacteria.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02801.x" xmlns="http://purl.org/rss/1.0/"><title>Self-Cleaning and Antibacteric Ceramic Tile Surface</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02801.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Self-Cleaning and Antibacteric Ceramic Tile Surface</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Simona Niederhãusern, Moreno Bondi, Federica Bondioli</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-09-17T11:36:30.045588-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02801.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02801.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02801.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The aim of this investigation was the surface functionalization of industrial ceramic tiles by sol-gel technique to improve at the same time the cleanability and the antibacterial activity of surfaces. This objective was pursued through the design and preparation of nanostructured titania-silver coating that was deposited on glazed, unglazed, and polished tiles by air-brushing. The obtained results showed that the applied coatings are transparent, show a good adhesion, and a remarkable antibacterial activity under the tested conditions. The surface photocatalicity was optimized with the higher thermal treatments (200°C) even if photodegradation process is clearly affected by the sample surface roughness.</p></div>
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The aim of this investigation was the surface functionalization of industrial ceramic tiles by sol-gel technique to improve at the same time the cleanability and the antibacterial activity of surfaces. This objective was pursued through the design and preparation of nanostructured titania-silver coating that was deposited on glazed, unglazed, and polished tiles by air-brushing. The obtained results showed that the applied coatings are transparent, show a good adhesion, and a remarkable antibacterial activity under the tested conditions. The surface photocatalicity was optimized with the higher thermal treatments (200°C) even if photodegradation process is clearly affected by the sample surface roughness.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02797.x" xmlns="http://purl.org/rss/1.0/"><title>Detection and Analysis of Crack Propagation in PZT Multilayer Ceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02797.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Detection and Analysis of Crack Propagation in PZT Multilayer Ceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Tobias Kühnlein, Alexander Klonczynski, Martin Rauscher</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-09-07T06:20:30.174646-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02797.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02797.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02797.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The flaw propagation in Lead zirconate titanate (PZT) multilayer ceramics under mechanical load was examined using impedance spectroscopy and three-point bending studies. Initial flaws were generated by applying a positive sinusoidal electric field to the specimens. The cracks were sequentially propagated and after the release of the external mechanical load, impedance spectroscopy was conducted. The shift in the resonance frequencies and the subresonance height of the impedance spectroscopy were used as a measure of flaw extension. A functional dependence of the resonance frequency and the phase shift on the crack length was found. The crack propagation was studied on flaws starting at the positive and negative electrode, respectively. The maximum fracture strength, as well as the crack path, depends on the electrode potential. The variation in the fracture strength was caused by different observed fracture mode: interface cracking, matrix-cracking, or a combination of both. The morphology of the fracture surfaces was ascribed to a textured microstructure, which is created by the sample processing, for example, by the poling process. A modified poling procedure with a lower poling temperature was analyzed, which yielded a reduction of the anisotropy of the electrode strength. Impedance spectroscopy was found to be a reliable measurement tool for automated flaw detection in PZT multilayer ceramics.</p></div>
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The flaw propagation in Lead zirconate titanate (PZT) multilayer ceramics under mechanical load was examined using impedance spectroscopy and three-point bending studies. Initial flaws were generated by applying a positive sinusoidal electric field to the specimens. The cracks were sequentially propagated and after the release of the external mechanical load, impedance spectroscopy was conducted. The shift in the resonance frequencies and the subresonance height of the impedance spectroscopy were used as a measure of flaw extension. A functional dependence of the resonance frequency and the phase shift on the crack length was found. The crack propagation was studied on flaws starting at the positive and negative electrode, respectively. The maximum fracture strength, as well as the crack path, depends on the electrode potential. The variation in the fracture strength was caused by different observed fracture mode: interface cracking, matrix-cracking, or a combination of both. The morphology of the fracture surfaces was ascribed to a textured microstructure, which is created by the sample processing, for example, by the poling process. A modified poling procedure with a lower poling temperature was analyzed, which yielded a reduction of the anisotropy of the electrode strength. Impedance spectroscopy was found to be a reliable measurement tool for automated flaw detection in PZT multilayer ceramics.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02794.x" xmlns="http://purl.org/rss/1.0/"><title>Effect of BBS-Based Frit on the Low Temperature Sintering and Electrical Properties of KNN Lead-Free Piezoceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02794.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of BBS-Based Frit on the Low Temperature Sintering and Electrical Properties of KNN Lead-Free Piezoceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yue-Ming Li, Zong-Yang Shen, Run-Run Li, Zhu-Mei Wang, Yan Hong, Run-Hua Liao</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-09-07T06:14:44.532471-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02794.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02794.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02794.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Using <span class="fixed-roman">BaO</span>–<span class="fixed-roman">B</span><sub>2</sub><span class="fixed-roman">O</span><sub>3</sub>–<span class="fixed-roman">SiO</span><sub>2</sub> (BBS)-based frit as sintering aid, the <span class="fixed-roman">K</span><sub>0.49</sub><span class="fixed-roman">Na</span><sub>0.51</sub><span class="fixed-roman">NbO</span><sub>3</sub> (KNN) + <em>x</em> wt% BBS (<em>x </em>=<em> </em>1.0, 1.5, 2.0 and 2.5) lead-free piezoelectric ceramics were successfully fabricated by solid-state reaction method under low-sintering temperature of 1000°C. The effect of BBS frit doping amount on the structure and electrical properties of the ceramics was investigated. The KNN ceramics with 1.5 wt% BBS frit showed optimal properties as follows: piezoelectric constant <em>d</em><sub>33</sub> = 108 pC/N, planar electromechanical coupling coefficient <em>k</em><sub>p</sub> = 41%, mechanical quality factor <em>Q</em><sub>m</sub> = 225, relative dielectric constant <em>ε</em><sub>r</sub> = 410, dielectric loss tan<em>δ</em> = 0.57% and Curie temperature <em>T</em><sub>c</sub> = 400°C. This ceramic sample should be a good lead-free candidate for actuators or high temperature sensors application due to its ultra-low tan<em>δ</em>, relatively high <em>Q</em><sub>m</sub> and <em>T</em><sub>c</sub>.</p></div>
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Using BaO–B2O3–SiO2 (BBS)-based frit as sintering aid, the K0.49Na0.51NbO3 (KNN) + x wt% BBS (x = 1.0, 1.5, 2.0 and 2.5) lead-free piezoelectric ceramics were successfully fabricated by solid-state reaction method under low-sintering temperature of 1000°C. The effect of BBS frit doping amount on the structure and electrical properties of the ceramics was investigated. The KNN ceramics with 1.5 wt% BBS frit showed optimal properties as follows: piezoelectric constant d33 = 108 pC/N, planar electromechanical coupling coefficient kp = 41%, mechanical quality factor Qm = 225, relative dielectric constant εr = 410, dielectric loss tanδ = 0.57% and Curie temperature Tc = 400°C. This ceramic sample should be a good lead-free candidate for actuators or high temperature sensors application due to its ultra-low tanδ, relatively high Qm and Tc.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02796.x" xmlns="http://purl.org/rss/1.0/"><title>Dielectric Properties and Low-Temperature Sintering of the Ba0.6Sr0.4TiO3 Ceramics with B2O3/CuO Additions</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02796.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Dielectric Properties and Low-Temperature Sintering of the Ba0.6Sr0.4TiO3 Ceramics with B2O3/CuO Additions</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hai Tao Jiang, Ji Wei Zhai, Jing Ji Zhang, Xi Yao</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-09-07T06:14:41.857793-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02796.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02796.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02796.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The sintering behaviors and dielectric properties of <span class="fixed-roman">Ba</span><sub>0.6</sub><span class="fixed-roman">Sr</span><sub>0.4</sub><span class="fixed-roman">TiO</span><sub>3</sub> ceramics were investigated as a function of <span class="fixed-roman">B</span><sub>2</sub><span class="fixed-roman">O</span><sub>3</sub> and <span class="fixed-roman">CuO</span> content. The addition of both <span class="fixed-roman">B</span><sub>2</sub><span class="fixed-roman">O</span><sub>3</sub> and <span class="fixed-roman">CuO</span> reduced the sintering temperature of <span class="fixed-roman">Ba</span><sub>0.6</sub><span class="fixed-roman">Sr</span><sub>0.4</sub><span class="fixed-roman">TiO</span><sub>3</sub> about 500°C. It was suggested that a liquid phase <span class="fixed-roman">BaCu</span>(<span class="fixed-roman">B</span><sub>2</sub><span class="fixed-roman">O</span><sub>5</sub>) was formed and assisted the densification of <span class="fixed-roman">Ba</span><sub>0.6</sub><span class="fixed-roman">Sr</span><sub>0.4</sub><span class="fixed-roman">TiO</span><sub>3</sub> ceramics. <span class="fixed-roman">Ba</span><sub>0.6</sub><span class="fixed-roman">Sr</span><sub>0.4</sub><span class="fixed-roman">TiO</span><sub>3</sub> ceramics co-doped with 3.0 mol% <span class="fixed-roman">B</span><sub>2</sub><span class="fixed-roman">O</span><sub>3</sub>, and 2.0 mol% <span class="fixed-roman">CuO</span>, sintered at 950°C for 5 h, had a dense microstructure and showed good microwave dielectric properties of a moderate dielectric constant (ε = 1048), low dielectric loss (0.0090) and high tunability (42.2%) at dc electric field of 30 kV/cm.</p></div>
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The sintering behaviors and dielectric properties of Ba0.6Sr0.4TiO3 ceramics were investigated as a function of B2O3 and CuO content. The addition of both B2O3 and CuO reduced the sintering temperature of Ba0.6Sr0.4TiO3 about 500°C. It was suggested that a liquid phase BaCu(B2O5) was formed and assisted the densification of Ba0.6Sr0.4TiO3 ceramics. Ba0.6Sr0.4TiO3 ceramics co-doped with 3.0 mol% B2O3, and 2.0 mol% CuO, sintered at 950°C for 5 h, had a dense microstructure and showed good microwave dielectric properties of a moderate dielectric constant (ε = 1048), low dielectric loss (0.0090) and high tunability (42.2%) at dc electric field of 30 kV/cm.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02828.x" xmlns="http://purl.org/rss/1.0/"><title>Effect of Impurities and LiF Additive in Hot-Pressed Transparent Magnesium Aluminate Spinel</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02828.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of Impurities and LiF Additive in Hot-Pressed Transparent Magnesium Aluminate Spinel</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Marc Rubat du Merac, Ivar E. Reimanis, Charlene Smith, Hans-Joachim Kleebe, Mathis M. Müller</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-08-29T13:30:51.035361-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02828.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02828.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02828.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The effect of impurities and <span class="fixed-roman">LiF</span> sintering additive on the microstructure and optical properties of hot-pressed transparent <span class="fixed-roman">MgAl</span><sub>2</sub><span class="fixed-roman">O</span><sub>4</sub> spinel was investigated. A lower and a higher purity powder were hot pressed with and without <span class="fixed-roman">LiF</span> and process parameters varied. Microstructure was examined using optical and electron microscopy, optical properties using spectrophotometry, and chemistry using various spectroscopic techniques. Impurities present in parts-per million were found to segregate at grain boundaries and form an amorphous phase, restricting grain growth and causing scatter and opacity. It was found that <span class="fixed-roman">LiF</span> reacts with impurities to form volatile species that can be removed with proper processing, resulting in larger grain size and increased transmittance. LiF also counteracts absorption caused by reduction of spinel, but results in <span class="fixed-roman">MgO</span> loss, grain boundary embrittlement, and if trapped in higher concentration, restricts grain growth and causes scatter and opacity.</p></div>
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The effect of impurities and LiF sintering additive on the microstructure and optical properties of hot-pressed transparent MgAl2O4 spinel was investigated. A lower and a higher purity powder were hot pressed with and without LiF and process parameters varied. Microstructure was examined using optical and electron microscopy, optical properties using spectrophotometry, and chemistry using various spectroscopic techniques. Impurities present in parts-per million were found to segregate at grain boundaries and form an amorphous phase, restricting grain growth and causing scatter and opacity. It was found that LiF reacts with impurities to form volatile species that can be removed with proper processing, resulting in larger grain size and increased transmittance. LiF also counteracts absorption caused by reduction of spinel, but results in MgO loss, grain boundary embrittlement, and if trapped in higher concentration, restricts grain growth and causes scatter and opacity.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02824.x" xmlns="http://purl.org/rss/1.0/"><title>Novel Fluorapatite-Forsterite Nanocomposite Powder for Oral Bone Defects</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02824.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Novel Fluorapatite-Forsterite Nanocomposite Powder for Oral Bone Defects</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Anoosha Forghani, Mahta Mapar, Mahshid Kharaziha, Mohammad H. Fathi, Mehrafarin Fesharaki</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-08-27T10:52:08.383607-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02824.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02824.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02824.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Failing implants lead to osseous defects. Guided tissue regeneration made of bioactive ceramics has been used to promote bone formation in osseous deformation. The aim of this study was to prepare and to characterize the fluorapatite/forsterite nanocomposite powder for treatment of oral bone defects. In this study, these composite powders with different contents of forsterite nanopowder were prepared via sol-gel process. Characterization of prepared nanocomposite powders and their cytotoxicity evaluation were done and compared with pure forsterite and fluorapatite powders. Results showed that nanocomposite powders with crystallite size of about 21–24 nm were fabricated successfully by gel calcination at 600°C. Besides the non-toxicity effects of powders, nanocomposite containing 20 wt% forsterite significantly increased cell viability compared with control groups. According to these results, these nanocomposite powders might be suitable as bioactive material for oral bone defect.</p></div>
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Failing implants lead to osseous defects. Guided tissue regeneration made of bioactive ceramics has been used to promote bone formation in osseous deformation. The aim of this study was to prepare and to characterize the fluorapatite/forsterite nanocomposite powder for treatment of oral bone defects. In this study, these composite powders with different contents of forsterite nanopowder were prepared via sol-gel process. Characterization of prepared nanocomposite powders and their cytotoxicity evaluation were done and compared with pure forsterite and fluorapatite powders. Results showed that nanocomposite powders with crystallite size of about 21–24 nm were fabricated successfully by gel calcination at 600°C. Besides the non-toxicity effects of powders, nanocomposite containing 20 wt% forsterite significantly increased cell viability compared with control groups. According to these results, these nanocomposite powders might be suitable as bioactive material for oral bone defect.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02833.x" xmlns="http://purl.org/rss/1.0/"><title>Structure and Corrosion Resistance of PEO Ceramic Coatings on AZ91D Mg Alloy Under Three Kinds of Power Modes</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02833.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Structure and Corrosion Resistance of PEO Ceramic Coatings on AZ91D Mg Alloy Under Three Kinds of Power Modes</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yanli Jiang, Zhenxing Yu, Qixing Xia, Yajun Zhang, Zhaohua Jiang, Zhongping Yao, Zhendong Wu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-08-27T10:52:02.72037-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02833.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02833.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02833.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Power mode is one of the most important factors in the plasma electrolytic oxidation (PEO) technique, which greatly influences the structure and performances of the prepared ceramic coatings. The aim of this work was to investigate effects of three kinds of power modes (constant voltage (Mode 1), constant current (Mode 2), and constant power (Mode 3)) on the structure and corrosion resistance of the PEO ceramic coatings containing <span class="fixed-roman">Ca</span> and <span class="fixed-roman">P</span> on AZ91D <span class="fixed-roman">Mg</span> alloy. The phase composition, morphology, and the element distribution of the coatings was studied using X-ray diffraction, scanning electron microscopy, and energy-dispersive spectroscopy, respectively. The electrochemical impedance spectrum was measured to evaluate the structure and the corrosion resistance. The polarizing curves were measured to evaluate the corrosion resistance. The results show that the coatings are of porous structure and mainly composed of <span class="fixed-roman">MgO</span>. The thickness and surface roughness of three kinds of coatings abide by the following sequences: Mode 1 &gt; Mode 2 &gt; Mode 3. By comparison, “equivalent circuit” mode <em>R</em><sub>s</sub>{<em>Q</em><sub>1</sub>[<em>R</em><sub>1</sub>(<em>Q</em><sub>2</sub><em>R</em><sub>2</sub>)]} is the most proper to reflect the structure of such coatings, including the surface roughness, the outer layer pore structure, and the inner layer structure. The coatings prepared under Mode 1 are of maximum thickness and high density, and therefore have the best general corrosion resistance. And the coatings prepared under Mode 3 are of the smallest surface roughness and higher density, which leads to the best pitting corrosion resistance.</p></div>
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Power mode is one of the most important factors in the plasma electrolytic oxidation (PEO) technique, which greatly influences the structure and performances of the prepared ceramic coatings. The aim of this work was to investigate effects of three kinds of power modes (constant voltage (Mode 1), constant current (Mode 2), and constant power (Mode 3)) on the structure and corrosion resistance of the PEO ceramic coatings containing Ca and P on AZ91D Mg alloy. The phase composition, morphology, and the element distribution of the coatings was studied using X-ray diffraction, scanning electron microscopy, and energy-dispersive spectroscopy, respectively. The electrochemical impedance spectrum was measured to evaluate the structure and the corrosion resistance. The polarizing curves were measured to evaluate the corrosion resistance. The results show that the coatings are of porous structure and mainly composed of MgO. The thickness and surface roughness of three kinds of coatings abide by the following sequences: Mode 1 &gt; Mode 2 &gt; Mode 3. By comparison, “equivalent circuit” mode Rs{Q1[R1(Q2R2)]} is the most proper to reflect the structure of such coatings, including the surface roughness, the outer layer pore structure, and the inner layer structure. The coatings prepared under Mode 1 are of maximum thickness and high density, and therefore have the best general corrosion resistance. And the coatings prepared under Mode 3 are of the smallest surface roughness and higher density, which leads to the best pitting corrosion resistance.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02829.x" xmlns="http://purl.org/rss/1.0/"><title>Structure and Gas-Sensing Behavior of Electrospun Titania-Doped Chromium Oxide Fibers</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02829.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Structure and Gas-Sensing Behavior of Electrospun Titania-Doped Chromium Oxide Fibers</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yangong Zheng, Jing Wang, Pengpeng Chen, Chunyan Li, Xiaogan Li</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-08-27T10:50:36.477492-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02829.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02829.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02829.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Titania-doped chromium oxide (CTO) can serve as an active gas-sensing material. It has been successful in commercial gas sensors due to its good gas-sensing performance and stability in humid environment; especially with respect of volatile organic compounds (VOCs). CTO fibers with reticular structure were prepared by electrospinning technology and the sensing behavior upon exposure to ethanol was characterized in this report. The gas sensors made of CTO fibers show a good response to ethanol and stability for a long term at operating temperature of 400°C. The experimental results have been analyzed and simulated using the response equations. The humidity effects on the sensor performance were also evaluated. The results indicate that the CTO fibers could be used in practical applications.</p></div>
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Titania-doped chromium oxide (CTO) can serve as an active gas-sensing material. It has been successful in commercial gas sensors due to its good gas-sensing performance and stability in humid environment; especially with respect of volatile organic compounds (VOCs). CTO fibers with reticular structure were prepared by electrospinning technology and the sensing behavior upon exposure to ethanol was characterized in this report. The gas sensors made of CTO fibers show a good response to ethanol and stability for a long term at operating temperature of 400°C. The experimental results have been analyzed and simulated using the response equations. The humidity effects on the sensor performance were also evaluated. The results indicate that the CTO fibers could be used in practical applications.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02826.x" xmlns="http://purl.org/rss/1.0/"><title>Enhanced Properties of Dense AlN Ceramics via in situ Reaction</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02826.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Enhanced Properties of Dense AlN Ceramics via in situ Reaction</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yongjie Zhao, Rongxia Huang, Heping Zhou, Sung-Soo Ryu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-08-27T10:50:34.048062-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02826.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02826.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02826.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A novel approach to prepare dense <span class="fixed-roman">AlN</span> ceramics with high thermal conductivity was proposed. The aluminum isopropoxide (AIP) was introduced to prepare dense <span class="fixed-roman">AlN</span> ceramics possessing enhanced thermal conductivity via <em>in situ</em> reaction. The effect of AIP and sintering temperatures on the microstructure and properties of <span class="fixed-roman">AlN</span> ceramics were investigated. Results indicate that AIP is beneficial for the densification of AlN ceramics, and particularly, when the addition of AIP reaches 1 wt%, the density and thermal conductivity could reach up to 3.29 g/cm<sup>3</sup>, 182 W/mK, respectively. Finally, the mechanism of the <em>in situ</em> reaction was proposed.</p></div>
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A novel approach to prepare dense AlN ceramics with high thermal conductivity was proposed. The aluminum isopropoxide (AIP) was introduced to prepare dense AlN ceramics possessing enhanced thermal conductivity via in situ reaction. The effect of AIP and sintering temperatures on the microstructure and properties of AlN ceramics were investigated. Results indicate that AIP is beneficial for the densification of AlN ceramics, and particularly, when the addition of AIP reaches 1 wt%, the density and thermal conductivity could reach up to 3.29 g/cm3, 182 W/mK, respectively. Finally, the mechanism of the in situ reaction was proposed.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02825.x" xmlns="http://purl.org/rss/1.0/"><title>Densification, Crystallization, and Dielectric Properties of AlN, BN, and Si3N4 Filler-Containing LTCC Materials</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02825.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Densification, Crystallization, and Dielectric Properties of AlN, BN, and Si3N4 Filler-Containing LTCC Materials</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Kyung Pyo Hong, Ik Jin Choi, Jae Woong Jung, Hong Rak Choi, Yong Soo Cho, Jiyeon Kwak, Dong Heon Kang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-08-27T10:50:30.386191-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02825.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02825.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02825.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Glass composite dielectrics consisting of calcium aluminoborosilicate glass and nitride fillers such as aluminum nitride, boron nitride, and silicon nitride (<span class="fixed-roman">AlN</span>, <span class="fixed-roman">BN</span>, and <span class="fixed-roman">Si</span><sub>3</sub><span class="fixed-roman">N</span><sub>4</sub>) were investigated. Densification and crystallization behavior depended on the type of filler, filler content, and firing temperature. <span class="fixed-roman">AlN</span> was most promising in generating desirable densification and dielectric properties (<em>k</em> of ~7.2 and tanδ of ~0.003) at 850°C with progressive crystallization of common anorthite phase. <span class="fixed-roman">BN</span> tended to show no significant densification and suppression of crystallization. <span class="fixed-roman">Si</span><sub>3</sub><span class="fixed-roman">N</span><sub>4</sub> resulted in abnormal behavior of densification, which can be highlighted with certain expansion at higher temperatures, as well as unexpected crystallization of <span class="fixed-roman">CaSiO</span><sub>3</sub> and <span class="fixed-roman">CaAl</span><sub>2</sub><span class="fixed-roman">SiO</span><sub>6</sub>.</p></div>
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Glass composite dielectrics consisting of calcium aluminoborosilicate glass and nitride fillers such as aluminum nitride, boron nitride, and silicon nitride (AlN, BN, and Si3N4) were investigated. Densification and crystallization behavior depended on the type of filler, filler content, and firing temperature. AlN was most promising in generating desirable densification and dielectric properties (k of ~7.2 and tanδ of ~0.003) at 850°C with progressive crystallization of common anorthite phase. BN tended to show no significant densification and suppression of crystallization. Si3N4 resulted in abnormal behavior of densification, which can be highlighted with certain expansion at higher temperatures, as well as unexpected crystallization of CaSiO3 and CaAl2SiO6.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02827.x" xmlns="http://purl.org/rss/1.0/"><title>Surface Characterization of γ-Al2O3 Powders and Their Co2+ Adsorption Properties</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02827.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Surface Characterization of γ-Al2O3 Powders and Their Co2+ Adsorption Properties</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Francisco Granados-Correa, Silvia Bulbulian</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-08-17T09:45:05.570743-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02827.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02827.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02827.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The relationship between structural and surface properties of γ-alumina prepared by various methods has been studied, and the adsorption ability of the powders for cobalt ions from aqueous solution is presented, based on the results of X-ray diffraction, specific surface area, scanning electron microscopy, and surface hydroxyl group concentration of the resulting products. Results show that γ-alumina obtained by solution-combustion method (specific surface area: 232.9 m<sup>2</sup>/g; morphology: lamellar and mesoporous; hydroxyl group content: 0.24 meq OH<sup>−</sup>/g) exhibited the best <span class="fixed-roman">Co</span><sup>2+</sup> adsorption. Furthermore, the synthesis of γ-alumina is highly helpful to study various structural and surface properties of this material.</p></div>
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The relationship between structural and surface properties of γ-alumina prepared by various methods has been studied, and the adsorption ability of the powders for cobalt ions from aqueous solution is presented, based on the results of X-ray diffraction, specific surface area, scanning electron microscopy, and surface hydroxyl group concentration of the resulting products. Results show that γ-alumina obtained by solution-combustion method (specific surface area: 232.9 m2/g; morphology: lamellar and mesoporous; hydroxyl group content: 0.24 meq OH−/g) exhibited the best Co2+ adsorption. Furthermore, the synthesis of γ-alumina is highly helpful to study various structural and surface properties of this material.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02810.x" xmlns="http://purl.org/rss/1.0/"><title>Support Vector Machine and Relevance Vector Machine for Prediction of Alumina and Pore Volume Fraction in Bioceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02810.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Support Vector Machine and Relevance Vector Machine for Prediction of Alumina and Pore Volume Fraction in Bioceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Kangeyanallore Govindaswamy Shanmugam Gopinath, Soumen Pal, Pijush Samui, Bimal Kumar Sarkar</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-08-06T10:33:55.23996-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02810.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02810.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02810.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The determination of wt% alumina (wa) and pore volume fraction (pv) in alumina-based bioceramics is important in ceramic engineering. This article adopts support vector machine (SVM) and relevance vector machine (RVM) for prediction of wa and pv based on SiC. SVM is firmly based on theory of statistical learning. RVM is based on a Bayesian formulation of a linear model with an appropriate prior that results in a sparse representation. The developed SVM and RVM give equations for prediction of wa and pv. This article gives robust models based on SVM and RVM for prediction of wa and pv.</p></div>
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The determination of wt% alumina (wa) and pore volume fraction (pv) in alumina-based bioceramics is important in ceramic engineering. This article adopts support vector machine (SVM) and relevance vector machine (RVM) for prediction of wa and pv based on SiC. SVM is firmly based on theory of statistical learning. RVM is based on a Bayesian formulation of a linear model with an appropriate prior that results in a sparse representation. The developed SVM and RVM give equations for prediction of wa and pv. This article gives robust models based on SVM and RVM for prediction of wa and pv.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02816.x" xmlns="http://purl.org/rss/1.0/"><title>Radio-Frequency Atmospheric-Pressure Plasma Synthesis of Ultrafine ZrC Powders</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02816.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Radio-Frequency Atmospheric-Pressure Plasma Synthesis of Ultrafine ZrC Powders</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Liuyang Bai, Haibao Zhang, Huacheng Jin, Fangli Yuan, Shulan Huang, Jinlin Li</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-07-25T14:51:29.853561-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02816.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02816.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02816.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A radio-frequency atmospheric-pressure plasma process has been applied to the synthesis of ultrafine <span class="fixed-roman">ZrC</span> powders using <span class="fixed-roman">ZrCl<sub>4</sub></span> and <span class="fixed-roman">CH<sub>4</sub></span> as precursors. Both thermodynamic analysis and experiments were conducted and the as-prepared samples were characterized by X-ray diffraction, electron microscopy, and laser scattering. Results showed that <span class="fixed-roman">ZrC</span> powders with particle size &lt;100 nm and surface area of 36.56 <em>M</em><sup>2</sup>/g could be obtained. The addition of excess <span class="fixed-roman">H<sub>2</sub></span> contributed to the increase in conversion rate. The conversion rate was about 65% when the carrier gas ratio (<span class="fixed-roman">H<sub>2</sub></span>/<span class="fixed-roman">CH<sub>4</sub></span>) was set at 4.0 and added axially through the injection probe.</p></div>]]></content:encoded><description>A radio-frequency atmospheric-pressure plasma process has been applied to the synthesis of ultrafine ZrC powders using ZrCl4 and CH4 as precursors. Both thermodynamic analysis and experiments were conducted and the as-prepared samples were characterized by X-ray diffraction, electron microscopy, and laser scattering. Results showed that ZrC powders with particle size &lt;100 nm and surface area of 36.56 M2/g could be obtained. The addition of excess H2 contributed to the increase in conversion rate. The conversion rate was about 65% when the carrier gas ratio (H2/CH4) was set at 4.0 and added axially through the injection probe.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02813.x" xmlns="http://purl.org/rss/1.0/"><title>Influence of Ethanol Amount During Washing on Deagglomeration of Co-Precipitated Calcined Nanocrystalline 3YSZ Powders</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02813.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Influence of Ethanol Amount During Washing on Deagglomeration of Co-Precipitated Calcined Nanocrystalline 3YSZ Powders</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sharanabasappa B. Patil, Ajay Kumar Jena, Parag Bhargava</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-07-25T14:50:38.528969-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02813.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02813.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02813.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Influence of ethanol treatment of co-precipitated yttrium–zirconium hydroxide on deagglomeration of calcined nano 3<span class="fixed-roman">YSZ</span> powder was studied. Results indicated that the amount of ethanol used in washing the zirconium hydroxide precipitate had a significant impact on the calcined powder characteristics. Different ratios of ethanol to the water contained within the precipitate were used during washing and the calcined nano 3<span class="fixed-roman">YSZ</span> powders were characterized in terms of BET specific surface area, tap density, pressure-displacement behavior during powder compaction, nanoindentation of green compacts, green and sintered body microstructures. The results indicated that a minimum ethanol amount of 2–3 times that of water in the precipitate was required to achieve superior deagglomeration of the calcined nano <span class="fixed-roman">YSZ</span> powders. The powders obtained by washing with optimum ethanol amount resulted in high green density and sintered density of compacts.</p></div>]]></content:encoded><description>Influence of ethanol treatment of co-precipitated yttrium–zirconium hydroxide on deagglomeration of calcined nano 3YSZ powder was studied. Results indicated that the amount of ethanol used in washing the zirconium hydroxide precipitate had a significant impact on the calcined powder characteristics. Different ratios of ethanol to the water contained within the precipitate were used during washing and the calcined nano 3YSZ powders were characterized in terms of BET specific surface area, tap density, pressure-displacement behavior during powder compaction, nanoindentation of green compacts, green and sintered body microstructures. The results indicated that a minimum ethanol amount of 2–3 times that of water in the precipitate was required to achieve superior deagglomeration of the calcined nano YSZ powders. The powders obtained by washing with optimum ethanol amount resulted in high green density and sintered density of compacts.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02815.x" xmlns="http://purl.org/rss/1.0/"><title>The Immobilization of Polyethylene Imine Nano and Microspheres on Glass Using High Intensity Ultrasound</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02815.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">The Immobilization of Polyethylene Imine Nano and Microspheres on Glass Using High Intensity Ultrasound</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ulyana Shimanovich, Artur Cavaco-Paulo, Aharon Gedanken</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-07-18T11:11:14.721759-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02815.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02815.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02815.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The present article describes the creation and immobilization of Polyethylene imine (PEI) capsules on a glass surface. The synthesis and deposition were accomplished by short-time (3 min) one-step reaction. The preparation and immobilization of PEI spheres, was carried out using an environmental friendly method, the ultrasonic emulsification. The ultrasonic technique enables to control size and fulfillment of the internal part of the immobilized PEI spheres. Moreover, the ultrasonic emulsification method showed 100% efficiency in PEI spheres creation, which means no residues of aqueous PEI and oil solvents remained in the reaction flask after the nanosphere's creation. The immobilized PEI spheres have sizes varied from 50 to 500 nm. The PEI spheres were successfully filled either with organic solvent (hydrophobic) or with water (hydrophilic). This method provides us the perspective for future encapsulation of varies molecules which have hydrophobic or hydrophilic nature.</p></div>]]></content:encoded><description>The present article describes the creation and immobilization of Polyethylene imine (PEI) capsules on a glass surface. The synthesis and deposition were accomplished by short-time (3 min) one-step reaction. The preparation and immobilization of PEI spheres, was carried out using an environmental friendly method, the ultrasonic emulsification. The ultrasonic technique enables to control size and fulfillment of the internal part of the immobilized PEI spheres. Moreover, the ultrasonic emulsification method showed 100% efficiency in PEI spheres creation, which means no residues of aqueous PEI and oil solvents remained in the reaction flask after the nanosphere's creation. The immobilized PEI spheres have sizes varied from 50 to 500 nm. The PEI spheres were successfully filled either with organic solvent (hydrophobic) or with water (hydrophilic). This method provides us the perspective for future encapsulation of varies molecules which have hydrophobic or hydrophilic nature.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02814.x" xmlns="http://purl.org/rss/1.0/"><title>The Influence of Chromium Oxide on the Sintering Behavior of Silicon Nitride</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02814.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">The Influence of Chromium Oxide on the Sintering Behavior of Silicon Nitride</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ali Alem, Martin D. Pugh</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-07-18T11:10:21.597728-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02814.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02814.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02814.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>In this study, pressureless sintering of silicon nitride via the addition of chromium oxide was investigated. Silicon nitride samples containing additives from the <span class="fixed-roman">Cr</span>–<span class="fixed-roman">Cr</span><sub>2</sub><span class="fixed-roman">O</span><sub>3</sub>–<span class="fixed-roman">SiO</span><sub>2</sub> system were sintered under different conditions. The phase transformation, the degree of densification and the <em>in situ</em> reactions between <span class="fixed-roman">Si</span><sub>3</sub><span class="fixed-roman">N</span><sub>4</sub> and chromium compounds were investigated and the reactions were validated thermodynamically. It was found that <span class="fixed-roman">Si</span><sub>3</sub><span class="fixed-roman">N</span><sub>4</sub> reacts with <span class="fixed-roman">Cr</span><sub>2</sub><span class="fixed-roman">O</span><sub>3</sub> and <span class="fixed-roman">Cr</span> and these <em>in situ</em> reactions lead to <span class="fixed-roman">Si</span><sub>3</sub><span class="fixed-roman">N</span><sub>4</sub> decomposition and consequently formation of a series of chromium silicides including <span class="fixed-roman">Cr</span><sub>3</sub><span class="fixed-roman">Si</span>,<span class="fixed-roman">Cr</span><sub>5</sub><span class="fixed-roman">Si</span>, and <span class="fixed-roman">CrSi</span><sub>2</sub>. Due to the presence of chromium silicides as liquid phases during sintering, the α-<span class="fixed-roman">Si</span><sub>3</sub><span class="fixed-roman">N</span><sub>4</sub> to β-<span class="fixed-roman">Si</span><sub>3</sub><span class="fixed-roman">N</span><sub>4</sub> phase transformation started around 1400°C and was completed around 1800°C. On the other hand, densification of <span class="fixed-roman">Si</span><sub>3</sub><span class="fixed-roman">N</span><sub>4</sub> samples with chromium oxide addition was not observed. The participation of <span class="fixed-roman">Cr</span><sub>2</sub><span class="fixed-roman">O</span><sub>3</sub> in these <em>in situ</em> reactions prevents sufficient formation of chromium silicate and leads to insufficient liquid phase with poor wettability during sintering, resulting in poor densification.</p></div>]]></content:encoded><description>In this study, pressureless sintering of silicon nitride via the addition of chromium oxide was investigated. Silicon nitride samples containing additives from the Cr–Cr2O3–SiO2 system were sintered under different conditions. The phase transformation, the degree of densification and the in situ reactions between Si3N4 and chromium compounds were investigated and the reactions were validated thermodynamically. It was found that Si3N4 reacts with Cr2O3 and Cr and these in situ reactions lead to Si3N4 decomposition and consequently formation of a series of chromium silicides including Cr3Si,Cr5Si, and CrSi2. Due to the presence of chromium silicides as liquid phases during sintering, the α-Si3N4 to β-Si3N4 phase transformation started around 1400°C and was completed around 1800°C. On the other hand, densification of Si3N4 samples with chromium oxide addition was not observed. The participation of Cr2O3 in these in situ reactions prevents sufficient formation of chromium silicate and leads to insufficient liquid phase with poor wettability during sintering, resulting in poor densification.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02804.x" xmlns="http://purl.org/rss/1.0/"><title>Effect of Boron Nitride (BN) on Luminescent Properties of Y3Al5O12:Ce Phosphors and their White Light-Emitting Diode Characteristics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02804.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of Boron Nitride (BN) on Luminescent Properties of Y3Al5O12:Ce Phosphors and their White Light-Emitting Diode Characteristics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Xiaojun Wang, Hailong Zhang, Yi Zhao, Xinjuan Liu, Huili Li, Zhejuan Zhang, Zhuo Sun</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-07-09T14:01:06.575961-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02804.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02804.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02804.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>This article reports a low-cost yellow-emitting <span class="fixed-roman">Y<sub>3</sub>Al<sub>5-<em>x</em></sub>B<sub><em>x</em></sub>O<sub>12-<em>x</em></sub>N<sub><em>x</em></sub></span>:<span class="fixed-roman">Ce<sup>3+</sup></span> phosphor with an enhanced luminescent intensity and excellent thermal stability for white light-emitting diodes (LEDs). It was synthesized by a simple gas-pressure sintering (GPS) process. The effect of B<sup>3+</sup>–N<sup>3−</sup> incorporation on the optical properties of <span class="fixed-roman">Y<sub>3</sub>Al<sub>5</sub>O<sub>12</sub></span>:<span class="fixed-roman">Ce<sup>3+</sup></span> phosphor was investigated. The addition of appropriate amounts of boron nitride (BN) leads to a marked increase in photoluminescent intensity and a slight shift of its emission spectra toward the blue region, which is assigned to the improved crystallinity and increased particle size. Especially, the prepared oxynitride phosphor does not exhibit any thermal quenching under high temperature, and the emission intensity at 250°C even increases up to 175% of that measured at 20°C. Finally, the white LED flat lamp with luminous efficiency as high as 101 lm/W, color rendering index of 72, and correlated color temperature of about 6600 K is successfully realized by using <span class="fixed-roman">YAG</span>:<span class="fixed-roman">Ce<sup>3+</sup></span> phosphor doped with 0.5 molar ratio BN, which is acceptable and promising for general indoor illuminations to replace fluorescent or incandescent lamps.</p></div>
]]></content:encoded><description>
This article reports a low-cost yellow-emitting Y3Al5-xBxO12-xNx:Ce3+ phosphor with an enhanced luminescent intensity and excellent thermal stability for white light-emitting diodes (LEDs). It was synthesized by a simple gas-pressure sintering (GPS) process. The effect of B3+–N3− incorporation on the optical properties of Y3Al5O12:Ce3+ phosphor was investigated. The addition of appropriate amounts of boron nitride (BN) leads to a marked increase in photoluminescent intensity and a slight shift of its emission spectra toward the blue region, which is assigned to the improved crystallinity and increased particle size. Especially, the prepared oxynitride phosphor does not exhibit any thermal quenching under high temperature, and the emission intensity at 250°C even increases up to 175% of that measured at 20°C. Finally, the white LED flat lamp with luminous efficiency as high as 101 lm/W, color rendering index of 72, and correlated color temperature of about 6600 K is successfully realized by using YAG:Ce3+ phosphor doped with 0.5 molar ratio BN, which is acceptable and promising for general indoor illuminations to replace fluorescent or incandescent lamps.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02809.x" xmlns="http://purl.org/rss/1.0/"><title>The Thermal Stability and Photoluminescence Degradation of Mn2+ in Fluorescent Lamp used BaMgAl10O17:Eu2+,Mn2+ Phosphor</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02809.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">The Thermal Stability and Photoluminescence Degradation of Mn2+ in Fluorescent Lamp used BaMgAl10O17:Eu2+,Mn2+ Phosphor</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jiachi Zhang, Meijiao Zhou, Bitao Liu, Yuhua Wang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-07-09T09:53:21.659664-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02809.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02809.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02809.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The thermal stability and photoluminescence degradation of Mn<sup>2+</sup> in fluorescent lamps used <span class="fixed-roman">BaMgAl</span><sub>10</sub><span class="fixed-roman">O</span><sub>17</sub>:<span class="fixed-roman">Eu</span><sup>2+</sup>,<span class="fixed-roman">Mn</span><sup>2+</sup> phosphor are investigated. The detection of impurity containing manganese with high valence demonstrates the oxidation of <span class="fixed-roman">Mn</span><sup>2+</sup> during baking process at 700°C and it partly leads to emission degradation of <span class="fixed-roman">Mn</span><sup>2+</sup>. The emission of <span class="fixed-roman">Mn</span><sup>2+</sup> mainly originates from the energy transfer of <span class="fixed-roman">Eu</span><sup>2+</sup>→<span class="fixed-roman">Mn</span><sup>2+</sup>. The oxidation of <span class="fixed-roman">Eu</span><sup>2+</sup> decrease the amount of <span class="fixed-roman">Eu</span><sup>2+</sup> centers and thus finally causes the degradation of <span class="fixed-roman">Mn</span><sup>2+</sup>. Some traps are revealed to be induced during baking process and it further weakens energy transfer efficiency of <span class="fixed-roman">Eu</span><sup>2+</sup>→<span class="fixed-roman">Mn</span><sup>2+</sup> and decreases the emission of <span class="fixed-roman">Mn</span><sup>2+</sup>.</p></div>]]></content:encoded><description>The thermal stability and photoluminescence degradation of Mn2+ in fluorescent lamps used BaMgAl10O17:Eu2+,Mn2+ phosphor are investigated. The detection of impurity containing manganese with high valence demonstrates the oxidation of Mn2+ during baking process at 700°C and it partly leads to emission degradation of Mn2+. The emission of Mn2+ mainly originates from the energy transfer of Eu2+→Mn2+. The oxidation of Eu2+ decrease the amount of Eu2+ centers and thus finally causes the degradation of Mn2+. Some traps are revealed to be induced during baking process and it further weakens energy transfer efficiency of Eu2+→Mn2+ and decreases the emission of Mn2+.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02808.x" xmlns="http://purl.org/rss/1.0/"><title>Dielectric and Pyroelectric Properties of Ferroelectric SBN–PVDF Composites Prepared by Hot-Uniaxial Press</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02808.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Dielectric and Pyroelectric Properties of Ferroelectric SBN–PVDF Composites Prepared by Hot-Uniaxial Press</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Naresh Kumar, Pawan Kumar</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-07-09T09:53:15.804906-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02808.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02808.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02808.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Composites of polyvinyledene fluoride (PVDF) and strontium barium niobate (<span class="fixed-roman">Sr</span><sub><em>x</em></sub><span class="fixed-roman">Ba</span><sub>1−<em>x</em></sub><span class="fixed-roman">Nb</span><sub>2</sub><span class="fixed-roman">O</span><sub>6</sub> for <em>x</em> = 0.53/<span class="fixed-roman">SBN</span>)/Ф<span class="fixed-roman">SBN</span> − (1 − Ф)PVDF with Ф = 0.1 to 0.3 have been prepared by hot uniaxial press. Structural, morphological, dielectric and pyrolectric properties of the composites have been studied. Self-sustaining thick films with a 0–3 connectivity have been synthesized. The dielectric constant (ε<sub>r</sub>) was found to increase with the increase in ceramic volume fraction (Ф) in the composite. The composite with Ф = 0.3 is found to have highest values of pyroelectric coefficient (p<sub>i</sub>) ~13.475 μC/m<sup>2</sup>K, FOM<sub>I</sub> ~0.481 μC/m<sup>2</sup>K and FOM<sub>II</sub> ~20.13 μC/m<sup>2</sup>K with good mechanical flexibility.</p></div>]]></content:encoded><description>Composites of polyvinyledene fluoride (PVDF) and strontium barium niobate (SrxBa1−xNb2O6 for x = 0.53/SBN)/ФSBN − (1 − Ф)PVDF with Ф = 0.1 to 0.3 have been prepared by hot uniaxial press. Structural, morphological, dielectric and pyrolectric properties of the composites have been studied. Self-sustaining thick films with a 0–3 connectivity have been synthesized. The dielectric constant (εr) was found to increase with the increase in ceramic volume fraction (Ф) in the composite. The composite with Ф = 0.3 is found to have highest values of pyroelectric coefficient (pi) ~13.475 μC/m2K, FOMI ~0.481 μC/m2K and FOMII ~20.13 μC/m2K with good mechanical flexibility.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02805.x" xmlns="http://purl.org/rss/1.0/"><title>Enhancement of Properties and Performance of MoSi2-based Heating Elements via Low Temperature Sintering</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02805.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Enhancement of Properties and Performance of MoSi2-based Heating Elements via Low Temperature Sintering</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jianying Gao, Lianjun Wang, Wan Jiang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-07-09T09:53:02.812-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02805.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02805.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02805.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Investigation on properties and performance of <span class="fixed-roman">MoSi<sub>2</sub></span>-based heating elements was carried out using high temperature sintering (HT), low-high temperature sintering (LHT), and low temperature sintering (LT) processes. Flexural strength depends proportionally on the thickness of protective surface scale, which is determined by the sintering temperature. The performance, indicated as critical damage temperature, is significantly correlated with the degree of densification, embodying dramatic deterioration with increasing porosity. LHT is more promising in industrially producing high-performance <span class="fixed-roman">MoSi<sub>2</sub></span>-based heating elements because of advantages in densification and efficiency compared with HT and LT.</p></div>]]></content:encoded><description>Investigation on properties and performance of MoSi2-based heating elements was carried out using high temperature sintering (HT), low-high temperature sintering (LHT), and low temperature sintering (LT) processes. Flexural strength depends proportionally on the thickness of protective surface scale, which is determined by the sintering temperature. The performance, indicated as critical damage temperature, is significantly correlated with the degree of densification, embodying dramatic deterioration with increasing porosity. LHT is more promising in industrially producing high-performance MoSi2-based heating elements because of advantages in densification and efficiency compared with HT and LT.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02799.x" xmlns="http://purl.org/rss/1.0/"><title>Hot-Pressing Method to Consolidate Gd3(Al,Ga)5O12:Ce Garnet Scintillator Powder for use in an X-ray CT Detector</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02799.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Hot-Pressing Method to Consolidate Gd3(Al,Ga)5O12:Ce Garnet Scintillator Powder for use in an X-ray CT Detector</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Tsuneyuki Kanai, Makoto Satoh, Ichiro Miura</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-06-29T13:50:49.482465-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02799.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02799.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02799.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>We have developed a hot-pressing method for consolidating garnet scintillator powder of composition <span class="fixed-roman">Gd</span><sub>3</sub>(<span class="fixed-roman">Al</span>,<span class="fixed-roman">Ga</span>)<sub>5</sub><span class="fixed-roman">O</span><sub>12</sub>:<span class="fixed-roman">Ce</span>. Thermodynamic analysis revealed that gallium oxide, which was a constituent of the garnet scintillator powder, would react with the graphite mold beginning at 950°C and would be reduced to gallium metal. To prevent this reaction during hot-pressing, a reaction barrier material was placed between the graphite mold and the scintillator powder. As for the reaction barrier material, 3<span class="fixed-roman">Gd</span><span class="fixed-roman">AlO</span><sub>3</sub>–<span class="fixed-roman">Al</span><sub>2</sub><span class="fixed-roman">O</span><sub>3</sub> powder calcined at 1100°C was found to be suitable because the material provided two important characteristics: the same thermal expansion coefficient as the scintillator material and good sinterability. The <span class="fixed-roman">Gd</span><sub>3</sub>(<span class="fixed-roman">Al</span>,<span class="fixed-roman">Ga</span>)<sub>5</sub><span class="fixed-roman">O</span><sub>12</sub>:Ce garnet scintillator powder was hot pressed at 1475°C for 4 h in vacuum, followed by annealing at 1300°C for 4 h in oxygen atmosphere. The thus obtained garnet scintillator successfully satisfied the necessary requirements for use in an X-ray computed tomography detector.</p></div>]]></content:encoded><description>We have developed a hot-pressing method for consolidating garnet scintillator powder of composition Gd3(Al,Ga)5O12:Ce. Thermodynamic analysis revealed that gallium oxide, which was a constituent of the garnet scintillator powder, would react with the graphite mold beginning at 950°C and would be reduced to gallium metal. To prevent this reaction during hot-pressing, a reaction barrier material was placed between the graphite mold and the scintillator powder. As for the reaction barrier material, 3GdAlO3–Al2O3 powder calcined at 1100°C was found to be suitable because the material provided two important characteristics: the same thermal expansion coefficient as the scintillator material and good sinterability. The Gd3(Al,Ga)5O12:Ce garnet scintillator powder was hot pressed at 1475°C for 4 h in vacuum, followed by annealing at 1300°C for 4 h in oxygen atmosphere. The thus obtained garnet scintillator successfully satisfied the necessary requirements for use in an X-ray computed tomography detector.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02803.x" xmlns="http://purl.org/rss/1.0/"><title>Dispersion and Gelcasting of Zirconium Diboride through Aqueous Route</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02803.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Dispersion and Gelcasting of Zirconium Diboride through Aqueous Route</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jie Yin, Xuejian Liu, Hui Zhang, Yongjie Yan, Zhengren Huang, Yong Yang, Dongliang Jiang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-06-29T13:50:30.677135-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02803.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02803.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02803.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The dispersion of highly concentrated Zirconium diboride (<span class="fixed-roman">ZrB</span><sub>2</sub>) suspension in aqueous media was investigated in terms of zeta potential and rheological measurements, with a salt of polyacrylate polymer (SD-07) as dispersant. The adsorption behavior of SD-07 on <span class="fixed-roman">ZrB</span><sub>2</sub> particle surface was also studied. Results showed that acid cleaning improved the fluidity of aqueous <span class="fixed-roman">ZrB</span><sub>2</sub> slurry. Concentrated (up to 50 vol%) and well-stabilized suspension was obtained in the alkaline pH region, with 0.60 mg/m<sup>2</sup> SD-07. On this basis, 50 vol% <span class="fixed-roman">ZrB</span><sub>2</sub> gelcasting slurry was prepared. The linear shrinkage and flexural strength of as-casted green body were (3.42 ± 0.13)% and (9.4 ± 0.3) MPa, respectively.</p></div>]]></content:encoded><description>The dispersion of highly concentrated Zirconium diboride (ZrB2) suspension in aqueous media was investigated in terms of zeta potential and rheological measurements, with a salt of polyacrylate polymer (SD-07) as dispersant. The adsorption behavior of SD-07 on ZrB2 particle surface was also studied. Results showed that acid cleaning improved the fluidity of aqueous ZrB2 slurry. Concentrated (up to 50 vol%) and well-stabilized suspension was obtained in the alkaline pH region, with 0.60 mg/m2 SD-07. On this basis, 50 vol% ZrB2 gelcasting slurry was prepared. The linear shrinkage and flexural strength of as-casted green body were (3.42 ± 0.13)% and (9.4 ± 0.3) MPa, respectively.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02800.x" xmlns="http://purl.org/rss/1.0/"><title>Morphology Control and Self-Setting Modification of α-Calcium Sulfate Hemihydrate Bone Cement by Addition of Ethanol</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02800.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Morphology Control and Self-Setting Modification of α-Calcium Sulfate Hemihydrate Bone Cement by Addition of Ethanol</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Zongyou Pan, Guangyong Yang, Yi Lou, Enxing Xue, Huazi Xu, Xigeng Miao, Jianli Liu, Chunfeng Hu, Qing Huang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-06-29T13:50:21.959245-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02800.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02800.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02800.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The self-setting behavior of α-calcium sulfate hemihydrate is highly dependent on its morphology that is tuned through the addition of ethanol into <span class="fixed-roman">CaCl<sub>2</sub></span> aqueous solutions during a salt solution method. With the increase of the ethanol/water volume ratios, the mean lengths of the formed crystals decreased from 24 to 19 μm, whereas their mean widths increased from 6 to 18 μm. It is also detected that the setting time of α-<span class="fixed-roman">CSH</span> paste reduced from 120 ± 12.3 to 17 ± 2.1 min as the crystal morphology evolved from rod-like to equiaxial.</p></div>]]></content:encoded><description>The self-setting behavior of α-calcium sulfate hemihydrate is highly dependent on its morphology that is tuned through the addition of ethanol into CaCl2 aqueous solutions during a salt solution method. With the increase of the ethanol/water volume ratios, the mean lengths of the formed crystals decreased from 24 to 19 μm, whereas their mean widths increased from 6 to 18 μm. It is also detected that the setting time of α-CSH paste reduced from 120 ± 12.3 to 17 ± 2.1 min as the crystal morphology evolved from rod-like to equiaxial.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02787.x" xmlns="http://purl.org/rss/1.0/"><title>Effect of MgO and PVA on the Synthesis and Properties of Negative Thermal Expansion Ceramics of Zr2(WO4)(PO4)2</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02787.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of MgO and PVA on the Synthesis and Properties of Negative Thermal Expansion Ceramics of Zr2(WO4)(PO4)2</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Rui Shang, Qinglun Hu, Xiansheng Liu, Erjun Liang, Bin Yuan, Mingju Chao</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-06-27T10:15:46.090839-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02787.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02787.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02787.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A green synthesis of Zr<sub>2</sub>(WO<sub>4</sub>)(PO<sub>4</sub>)<sub>2</sub> ceramics from ZrO<sub>2</sub>, WO<sub>3</sub> and P<sub>2</sub>O<sub>5</sub> is presented. It is shown that the ceramics can be synthesized by one-step sintering within 60 min. The relative density of the ceramics can be enhanced from about 75% without sintering additives to 99.8% of the theoretical value with 1.0 wt% MgO and 2.0 wt% polyvinyl alcohol. The grain sizes of the ceramics are smaller and more uniform with MgO added in the raw materials than with MgO added in the Zr<sub>2</sub>(WO<sub>4</sub>)(PO<sub>4</sub>)<sub>2</sub> powder. The coefficients of thermal expansion are about −2.325 × 10<sup>−6</sup>, −1.406 × 10<sup>−6</sup>, −1.509 × 10<sup>−6</sup> and −1.384 × 10<sup>−6</sup>°C<sup>−1</sup> for the samples without MgO, with MgO added in the raw materials, with MgO added in the Zr<sub>2</sub>(WO<sub>4</sub>)(PO<sub>4</sub>)<sub>2</sub> powder and with MgO and PVA added in the raw materials, respectively.</p></div>]]></content:encoded><description>A green synthesis of Zr2(WO4)(PO4)2 ceramics from ZrO2, WO3 and P2O5 is presented. It is shown that the ceramics can be synthesized by one-step sintering within 60 min. The relative density of the ceramics can be enhanced from about 75% without sintering additives to 99.8% of the theoretical value with 1.0 wt% MgO and 2.0 wt% polyvinyl alcohol. The grain sizes of the ceramics are smaller and more uniform with MgO added in the raw materials than with MgO added in the Zr2(WO4)(PO4)2 powder. The coefficients of thermal expansion are about −2.325 × 10−6, −1.406 × 10−6, −1.509 × 10−6 and −1.384 × 10−6°C−1 for the samples without MgO, with MgO added in the raw materials, with MgO added in the Zr2(WO4)(PO4)2 powder and with MgO and PVA added in the raw materials, respectively.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02793.x" xmlns="http://purl.org/rss/1.0/"><title>Low-Temperature Sintering and Microwave Dielectric Properties of ZnNb2O6–TiO2 Ceramics with BaCu(B2O5) Additions</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02793.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Low-Temperature Sintering and Microwave Dielectric Properties of ZnNb2O6–TiO2 Ceramics with BaCu(B2O5) Additions</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mei Guo, Gang Dou, Shuping Gong, Dongxiang Zhou</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-05-24T04:35:54.255048-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02793.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02793.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02793.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The influence of <span class="fixed-roman">BaCu</span>(<span class="fixed-roman">B</span><sub>2</sub><span class="fixed-roman">O</span><sub>5</sub>) (BCB) on densification, phases, microstructure and microwave dielectric properties of <span class="fixed-roman">ZnNb</span><sub>2</sub><span class="fixed-roman">O</span><sub>6</sub>–<em>x</em><span class="fixed-roman">TiO</span><sub>2</sub> (<em>x</em> = 1.70–1.90) composite ceramics have been investigated. Undoped <span class="fixed-roman">ZnNb</span><sub>2</sub><span class="fixed-roman">O</span><sub>6</sub>–1.8<span class="fixed-roman">TiO</span><sub>2</sub> ceramics sintered at 1200°C exhibit temperature coefficient of resonant frequency (<em>τ</em><sub><em>f</em></sub>) ~9.25 ppm/°C. When <span class="fixed-roman">BaCu</span>(<span class="fixed-roman">B</span><sub>2</sub><span class="fixed-roman">O</span><sub>5</sub>) was added, the sintering temperature of the <span class="fixed-roman">ZnNb</span><sub>2</sub><span class="fixed-roman">O</span><sub>6</sub>–1.8<span class="fixed-roman">TiO</span><sub>2</sub> composite ceramics was effectively reduced to 950°C. The results indicated that the permittivity and <em>Q</em> × <em>f</em> were dependent on the sintering temperature and the amounts of <span class="fixed-roman">BaCu</span>(<span class="fixed-roman">B</span><sub>2</sub><span class="fixed-roman">O</span><sub>5</sub>). Addition of 3.0 wt% <span class="fixed-roman">BaCu</span>(<span class="fixed-roman">B</span><sub>2</sub><span class="fixed-roman">O</span><sub>5</sub>) in <span class="fixed-roman">ZnNb</span><sub>2</sub><span class="fixed-roman">O</span><sub>6</sub>–1.8<span class="fixed-roman">TiO</span><sub>2</sub> ceramics sintered at 950°C showed excellent dielectric properties of <em>ε</em><sub><em>r</em></sub> = 40.9, <em>Q</em> × <em>f</em> = 12,200 GHz (<em>f</em> = 5.015 GHz) and <em>τ</em><sub><em>f</em></sub> = +0.3 ppm/°C.</p></div>]]></content:encoded><description>The influence of BaCu(B2O5) (BCB) on densification, phases, microstructure and microwave dielectric properties of ZnNb2O6–xTiO2 (x = 1.70–1.90) composite ceramics have been investigated. Undoped ZnNb2O6–1.8TiO2 ceramics sintered at 1200°C exhibit temperature coefficient of resonant frequency (τf) ~9.25 ppm/°C. When BaCu(B2O5) was added, the sintering temperature of the ZnNb2O6–1.8TiO2 composite ceramics was effectively reduced to 950°C. The results indicated that the permittivity and Q × f were dependent on the sintering temperature and the amounts of BaCu(B2O5). Addition of 3.0 wt% BaCu(B2O5) in ZnNb2O6–1.8TiO2 ceramics sintered at 950°C showed excellent dielectric properties of εr = 40.9, Q × f = 12,200 GHz (f = 5.015 GHz) and τf = +0.3 ppm/°C.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02782.x" xmlns="http://purl.org/rss/1.0/"><title>Sintering and Dielectric Properties of Li2O–B2O3–Al2O3–SiO2 Glass-Added (Ca0.7Sr0.3O)1.03(Ti0.1Zr0.9)O2 for Copper Electrode</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02782.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Sintering and Dielectric Properties of Li2O–B2O3–Al2O3–SiO2 Glass-Added (Ca0.7Sr0.3O)1.03(Ti0.1Zr0.9)O2 for Copper Electrode</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hyunho Shin, Sang-Wook Lee, Hyun Suk Jung</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-04-18T10:25:38.558492-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02782.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02782.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02782.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>When 1.5 wt% of <span class="fixed-roman">Li<sub>2</sub>O</span>–<span class="fixed-roman">B<sub>2</sub>O<sub>3</sub></span>–<span class="fixed-roman">SiO<sub>2</sub></span> and 1.5 wt% of <span class="fixed-roman">Li<sub>2</sub>O</span>–<span class="fixed-roman">B<sub>2</sub>O<sub>3</sub></span>–<span class="fixed-roman">Al<sub>2</sub>O<sub>3</sub></span> glass-added (<span class="fixed-roman">Ca</span><sub>0.7</sub><span class="fixed-roman">Sr</span><sub>0.3</sub><span class="fixed-roman">O</span>)<sub>1.03</sub>(<span class="fixed-roman">Ti</span><sub>0.1</sub><span class="fixed-roman">Zr</span><sub>0.9</sub>)<span class="fixed-roman">O</span><sub>2</sub> batch was ball milled for 10~30 h followed by sintering at 950°C in flowing <span class="fixed-roman">N</span><sub>2</sub>-10%<span class="fixed-roman">H</span><sub>2</sub> atmosphere, an apparent density of approximately 4.5 g/cm<sup>3</sup>, a dielectric constant of approximately 26, and a quality factor of roughly about 3300 GHz were demonstrated. A prolonged ball mill time thereafter significantly decreased both of the dielectric properties because of the enhanced reduction of the specimens during sintering. The apparent evidence of a material reaction between the dielectric material and the copper electrode was not observed.</p></div>]]></content:encoded><description>When 1.5 wt% of Li2O–B2O3–SiO2 and 1.5 wt% of Li2O–B2O3–Al2O3 glass-added (Ca0.7Sr0.3O)1.03(Ti0.1Zr0.9)O2 batch was ball milled for 10~30 h followed by sintering at 950°C in flowing N2-10%H2 atmosphere, an apparent density of approximately 4.5 g/cm3, a dielectric constant of approximately 26, and a quality factor of roughly about 3300 GHz were demonstrated. A prolonged ball mill time thereafter significantly decreased both of the dielectric properties because of the enhanced reduction of the specimens during sintering. The apparent evidence of a material reaction between the dielectric material and the copper electrode was not observed.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02772.x" xmlns="http://purl.org/rss/1.0/"><title>Synthesis of Alkali Aluminosilicates — Materials for Alkali Contaminated Environments at High Temperatures</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02772.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Synthesis of Alkali Aluminosilicates — Materials for Alkali Contaminated Environments at High Temperatures</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Nora Brachhold, Christos G. Aneziris</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-04-10T14:20:42.203848-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02772.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02772.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02772.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Alkali corrosion has become a problem in industrial furnaces especially because of the increasing use of secondary fuels. In the corroded lining material alkali aluminosilicates such as kalsilite, leucite or nepheline could be identified. According to ternary phase diagrams these substances have very high melting points which would make them suitable for high temperature applications in alkali corrosive environments. This study presents systematic synthesis experiments to produce alkali aluminosilicates by thermal (800°C, 1000°C, 1200°C) and hydrothermal (200°C) treatment starting from the nominal compositions of KAlSi<sub>2</sub>O<sub>6</sub>, KAlSiO<sub>4</sub>, and NaAlSiO<sub>4</sub>., KOH NaOH, quartz powder, and Al(OH)<sub>3</sub> were used as raw materials. The phase composition was analyzed by using X-ray diffraction (XRD). The alkali corrosion was tested using alkali salts as corrosive substances. The synthesis experiments resulted in multiphase reaction products. The hydrothermal method yielded only for the initial composition according to the stoichiometry of KAlSiO<sub>4</sub> crystalline phases of the same composition. The thermal method produced for all sets of synthesizing parameters mixtures of stoichiometric and nonstoichiometric alkali aluminosilicates. In the corrosion test, material of the nominal composition of KAlSiO<sub>4</sub> showed the best results. The material was corrosion resistant independently from the initially applied synthesizing parameters.</p></div>]]></content:encoded><description>Alkali corrosion has become a problem in industrial furnaces especially because of the increasing use of secondary fuels. In the corroded lining material alkali aluminosilicates such as kalsilite, leucite or nepheline could be identified. According to ternary phase diagrams these substances have very high melting points which would make them suitable for high temperature applications in alkali corrosive environments. This study presents systematic synthesis experiments to produce alkali aluminosilicates by thermal (800°C, 1000°C, 1200°C) and hydrothermal (200°C) treatment starting from the nominal compositions of KAlSi2O6, KAlSiO4, and NaAlSiO4., KOH NaOH, quartz powder, and Al(OH)3 were used as raw materials. The phase composition was analyzed by using X-ray diffraction (XRD). The alkali corrosion was tested using alkali salts as corrosive substances. The synthesis experiments resulted in multiphase reaction products. The hydrothermal method yielded only for the initial composition according to the stoichiometry of KAlSiO4 crystalline phases of the same composition. The thermal method produced for all sets of synthesizing parameters mixtures of stoichiometric and nonstoichiometric alkali aluminosilicates. In the corrosion test, material of the nominal composition of KAlSiO4 showed the best results. The material was corrosion resistant independently from the initially applied synthesizing parameters.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02771.x" xmlns="http://purl.org/rss/1.0/"><title>Effects of LiF on the Structure and Properties of Ba0.85Ca0.15Zr0.1Ti0.9O3 Lead-Free Piezoelectric Ceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02771.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effects of LiF on the Structure and Properties of Ba0.85Ca0.15Zr0.1Ti0.9O3 Lead-Free Piezoelectric Ceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Chee Kiang Ivan Tan, Kui Yao, Jan Ma</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-03-30T11:40:48.539336-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02771.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02771.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02771.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Preparation of Ba<sub>0.85</sub>Ca<sub>0.15</sub>Zr<sub>0.1</sub>Ti<sub>0.9</sub>O<sub>3</sub> (BCZT) lead-free piezoelectric ceramics with different amounts of LiF (BCZT-xLiF) was done, and the effects of the LiF doping on the phase transition behavior and the electrical properties of the resulting ceramic were investigated. The experimental results showed that the polymorphic rhombohedral-tetragonal phase transition temperature was found shifted toward room temperature with the Li doping. The study showed that BCZT lead-free piezoelectric ceramic with improved performance properties at room temperature can be achieved by shifting the polymorphic phase transition point nearer room temperature through the addition of LiF.</p></div>]]></content:encoded><description>Preparation of Ba0.85Ca0.15Zr0.1Ti0.9O3 (BCZT) lead-free piezoelectric ceramics with different amounts of LiF (BCZT-xLiF) was done, and the effects of the LiF doping on the phase transition behavior and the electrical properties of the resulting ceramic were investigated. The experimental results showed that the polymorphic rhombohedral-tetragonal phase transition temperature was found shifted toward room temperature with the Li doping. The study showed that BCZT lead-free piezoelectric ceramic with improved performance properties at room temperature can be achieved by shifting the polymorphic phase transition point nearer room temperature through the addition of LiF.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02767.x" xmlns="http://purl.org/rss/1.0/"><title>Effects of Impurity Iron Content on Characteristics of Sintered Reaction-Bonded Silicon Nitride</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02767.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effects of Impurity Iron Content on Characteristics of Sintered Reaction-Bonded Silicon Nitride</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dai Kusano, Yamato Noda, Hitomi Shibasaki, Hideki Hyuga, You Zhou, Kiyoshi Hirao</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-03-30T11:39:01.487314-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02767.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02767.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02767.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The effects of impurity iron content on characteristics of sintered reaction-bonded silicon nitrides were examined by adding iron powder to a high purity raw <span class="fixed-roman">Si</span> powder. Powder compacts of the raw <span class="fixed-roman">Si</span> powder doped with 2 mol% <span class="fixed-roman">Y<sub>2</sub>O<sub>3</sub></span> and 5 mol% <span class="fixed-roman">MgSiN<sub>2</sub></span> as sintering additives and <span class="fixed-roman">Fe</span> as impurity (0 mass%, 0.1 mass%, 1.0 mass% and 5.0 mass%) were nitrided at 1400°C for 8 h under a <span class="fixed-roman">N<sub>2</sub></span> pressure of 0.1 MPa, followed by post-sintering at 1900°C for 6 h under a <span class="fixed-roman">N<sub>2</sub></span> pressure of 0.9 MPa. All the SRBSN (Sintered Reaction-Bonded Silicon Nitride) specimens had about the same 4-point bending strength of 730–770 MPa. The fracture toughness of the specimens was gradually decreased with increasing Fe additive amount due to the inhibition of development of rodlike β-<span class="fixed-roman">Si<sub>3</sub>N<sub>4</sub></span> grains by <span class="fixed-roman">SiFe<sub>x</sub></span> particles formed during nitridation process. The thermal conductivity was also decreased with an increase in <span class="fixed-roman">Fe</span> amount. It seems that the increasing oxygen in grain-boundary phase caused by the oxidation of Fe during milling resulted in the increase in lattice oxygen of β-<span class="fixed-roman">Si<sub>3</sub>N<sub>4</sub></span> grains, which caused phonon scattering and thereby decreased thermal conductivity of β-<span class="fixed-roman">Si<sub>3</sub>N<sub>4</sub></span>. There was little change in the dielectric breakdown strength of the specimens: 24, 22, 22, and 21 kV/mm for the specimens without <span class="fixed-roman">Fe</span>, and with 0.1 mass%, 1.0 mass% and 5.0 mass% <span class="fixed-roman">Fe</span>, respectively. The surface resistivity of the specimens with 0 mass%, 0.1 mass% and 1.0 mass% <span class="fixed-roman">Fe</span> was in the range of 10<sup>13</sup> Ω, but the specimen with 5 mass% <span class="fixed-roman">Fe</span> was about one order lower than the others.</p></div>]]></content:encoded><description>The effects of impurity iron content on characteristics of sintered reaction-bonded silicon nitrides were examined by adding iron powder to a high purity raw Si powder. Powder compacts of the raw Si powder doped with 2 mol% Y2O3 and 5 mol% MgSiN2 as sintering additives and Fe as impurity (0 mass%, 0.1 mass%, 1.0 mass% and 5.0 mass%) were nitrided at 1400°C for 8 h under a N2 pressure of 0.1 MPa, followed by post-sintering at 1900°C for 6 h under a N2 pressure of 0.9 MPa. All the SRBSN (Sintered Reaction-Bonded Silicon Nitride) specimens had about the same 4-point bending strength of 730–770 MPa. The fracture toughness of the specimens was gradually decreased with increasing Fe additive amount due to the inhibition of development of rodlike β-Si3N4 grains by SiFex particles formed during nitridation process. The thermal conductivity was also decreased with an increase in Fe amount. It seems that the increasing oxygen in grain-boundary phase caused by the oxidation of Fe during milling resulted in the increase in lattice oxygen of β-Si3N4 grains, which caused phonon scattering and thereby decreased thermal conductivity of β-Si3N4. There was little change in the dielectric breakdown strength of the specimens: 24, 22, 22, and 21 kV/mm for the specimens without Fe, and with 0.1 mass%, 1.0 mass% and 5.0 mass% Fe, respectively. The surface resistivity of the specimens with 0 mass%, 0.1 mass% and 1.0 mass% Fe was in the range of 1013 Ω, but the specimen with 5 mass% Fe was about one order lower than the others.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02765.x" xmlns="http://purl.org/rss/1.0/"><title>Piezoelectric and Pyroelectric Materials Selection</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02765.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Piezoelectric and Pyroelectric Materials Selection</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Rahul Vaish</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-03-27T04:32:04.710402-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02765.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02765.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02765.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>An attempt has been made to provide the ranking of piezoelectric and pyroelectric materials using technique for order preference by similarity to ideal solution (TOPSIS) method. To calculate weight (priority) for all the attributes (properties) understudy, entropy method is used. Interestingly my results suggest that dielectric constant is a key parameter (after <em>d</em><sub>33</sub> coefficient) which governs selection of piezoelectric materials. PLZT (8/65/35) and LiTaO<sub>3</sub> ceramics place on first rank among studied piezoelectric and pyroelectric materials, respectively. These materials are classified using hierarchical clustering which shows similarities between the materials irrespective to their ranking obtained using TOPSIS method.</p></div>]]></content:encoded><description>An attempt has been made to provide the ranking of piezoelectric and pyroelectric materials using technique for order preference by similarity to ideal solution (TOPSIS) method. To calculate weight (priority) for all the attributes (properties) understudy, entropy method is used. Interestingly my results suggest that dielectric constant is a key parameter (after d33 coefficient) which governs selection of piezoelectric materials. PLZT (8/65/35) and LiTaO3 ceramics place on first rank among studied piezoelectric and pyroelectric materials, respectively. These materials are classified using hierarchical clustering which shows similarities between the materials irrespective to their ranking obtained using TOPSIS method.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02762.x" xmlns="http://purl.org/rss/1.0/"><title>Improvement of Mullite and Magnesia-Based Refractory Castables Through Addition of Nano-Spinel Powder</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02762.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Improvement of Mullite and Magnesia-Based Refractory Castables Through Addition of Nano-Spinel Powder</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Nagy M. Khalil, Mohamed M. S. Wahsh, Emad M. M. Ewais, Mohamed B. Hassan, S. M. Mehrez</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-03-15T13:42:21.377758-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02762.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02762.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02762.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Two different commercial refractory castables based on mullite or magnesia aggregates have been improved through addition of 0–25 wt.% nano-magnesium aluminate spinel (MA) powder. Physico-mechanical and refractory properties were tested at different firing temperatures. The phase composition, thermal analysis, and microstructure of these refractory castables were detected using X-ray diffraction (XRD), differential thermal analysis (DTA), as well as scanning electron microscope (SEM) attached with energy dispersive X-ray unit, respectively. The castable sample mix containing 10 wt.% nano-MA spinel powder was chosen as an optimum composition according to its good sintering, mechanical as well as refractory properties.</p></div>]]></content:encoded><description>Two different commercial refractory castables based on mullite or magnesia aggregates have been improved through addition of 0–25 wt.% nano-magnesium aluminate spinel (MA) powder. Physico-mechanical and refractory properties were tested at different firing temperatures. The phase composition, thermal analysis, and microstructure of these refractory castables were detected using X-ray diffraction (XRD), differential thermal analysis (DTA), as well as scanning electron microscope (SEM) attached with energy dispersive X-ray unit, respectively. The castable sample mix containing 10 wt.% nano-MA spinel powder was chosen as an optimum composition according to its good sintering, mechanical as well as refractory properties.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02763.x" xmlns="http://purl.org/rss/1.0/"><title>Application of Design of the Experiment in Preliminary Investigations on the end Milling of Low Temperature Co-fired Ceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02763.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Application of Design of the Experiment in Preliminary Investigations on the end Milling of Low Temperature Co-fired Ceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dominik Jurków, Leszek Golonka</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-03-08T12:27:56.666859-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02763.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02763.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02763.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The formation of three-dimensional shapes is one of the most important technological steps in low temperature co-fired ceramics (LTCC) process. Channels and chambers qualities and the process speed are strongly affected by the shaping procedure. There are three main machining techniques: laser cutting, punching, and milling. This article is dedicated to end milling process of LTCC tapes. The determined PS/DK 2<sup>3</sup> experiment design was used in the investigations and its procedure is described in this article. The used procedure is a very flexible method to achieve much useful information about the influence of the process parameters on the output. The PS/DK 2<sup>3</sup> experiment design enables analysis of the influence of: the three input parameters on the output (minimal obtained feature) and the interaction between the input parameters on the output (minimal obtained feature). Moreover, PS/DK 2<sup>3</sup> experiment design enables to obtain the mathematical model of the milling process and to decrease the number of measurements demanded to achieve the correct model. Hence, the design is suitable to decrease the time and costs of the experiment. The influence of the following input parameters: spindle rotational speed, spindle feed rate, vertical spindle step, and cutter diameter on minimal obtained feature of LTCC tapes is analyzed in this article.</p></div>]]></content:encoded><description>The formation of three-dimensional shapes is one of the most important technological steps in low temperature co-fired ceramics (LTCC) process. Channels and chambers qualities and the process speed are strongly affected by the shaping procedure. There are three main machining techniques: laser cutting, punching, and milling. This article is dedicated to end milling process of LTCC tapes. The determined PS/DK 23 experiment design was used in the investigations and its procedure is described in this article. The used procedure is a very flexible method to achieve much useful information about the influence of the process parameters on the output. The PS/DK 23 experiment design enables analysis of the influence of: the three input parameters on the output (minimal obtained feature) and the interaction between the input parameters on the output (minimal obtained feature). Moreover, PS/DK 23 experiment design enables to obtain the mathematical model of the milling process and to decrease the number of measurements demanded to achieve the correct model. Hence, the design is suitable to decrease the time and costs of the experiment. The influence of the following input parameters: spindle rotational speed, spindle feed rate, vertical spindle step, and cutter diameter on minimal obtained feature of LTCC tapes is analyzed in this article.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.0202728.x" xmlns="http://purl.org/rss/1.0/"><title>Titania Nanoparticle Suspension for Fabrication of Micrometer Feature Arrays via a Template-Assisted Approach</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.0202728.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Titania Nanoparticle Suspension for Fabrication of Micrometer Feature Arrays via a Template-Assisted Approach</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yongxuan Liang, Kathy Lu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-30T09:34:40.430025-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.0202728.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.0202728.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.0202728.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>In this study, <span class="fixed-roman">TiO</span><sub>2</sub> nanoparticle suspensions are guided by templated molds to fabricate micrometer feature patterns and arrays. The effects of PEG with different molecular weights on suspension flowability and surface wettability between the PDMS molds and the <span class="fixed-roman">TiO</span><sub>2</sub> suspensions on pattern formation are investigated. PEG 400 is the most desirable dispersant. The suspensions have the best wetting on the mold surface with 3 wt% TX-100 addition. Micrometer feature arrays with feature sizes ranging from 750 nm to 1.5 μm are obtained. Fundamental understanding, regarding suspension flowability, wetting, and the ability to make different feature sizes and shapes, is discussed.</p></div>]]></content:encoded><description>In this study, TiO2 nanoparticle suspensions are guided by templated molds to fabricate micrometer feature patterns and arrays. The effects of PEG with different molecular weights on suspension flowability and surface wettability between the PDMS molds and the TiO2 suspensions on pattern formation are investigated. PEG 400 is the most desirable dispersant. The suspensions have the best wetting on the mold surface with 3 wt% TX-100 addition. Micrometer feature arrays with feature sizes ranging from 750 nm to 1.5 μm are obtained. Fundamental understanding, regarding suspension flowability, wetting, and the ability to make different feature sizes and shapes, is discussed.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00709.x" xmlns="http://purl.org/rss/1.0/"><title>Fabrication of Full-Density Mg-Ferrite/Fe–Ni Permalloy Nanocomposites with a High-Saturation Magnetization Density of 1 T</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00709.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Fabrication of Full-Density Mg-Ferrite/Fe–Ni Permalloy Nanocomposites with a High-Saturation Magnetization Density of 1 T</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ken Hirota, Motoki Obatal; and?&gt;, Masaki Kato, Hideki Taguchi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-06T13:07:27.381153-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00709.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00709.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00709.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Dense nanocomposites consisting of spinel Mn-doped <span class="fixed-roman">Mg</span>-ferrite and permalloy, (<span class="fixed-roman">Mg</span>[<span class="fixed-roman">Fe</span><sub>1 − <em>x</em></sub><span class="fixed-roman">Mn</span><sub><em>x</em></sub>]<sub>2</sub><span class="fixed-roman">O</span><sub>4</sub>(0 ≤ <em>x</em> ≤ 0.4)/53<span class="fixed-roman">Fe</span>–47<span class="fixed-roman">Ni</span>), have been fabricated from powder mixtures of MgO/α-<span class="fixed-roman">Fe</span><sub>2</sub><span class="fixed-roman">O</span><sub>3</sub>/<span class="fixed-roman">MnO</span> and <span class="fixed-roman">N</span><sub>2</sub>-atomized metal particles utilizing high-pressure cold isostatic press (CIP), pulsed electric current pressure sintering (PECPS), and capsule-free hot isostatic pressing (HIP). Metal particles were coated with the mixed oxide powders homogeneously under high shear compression in Ar. The coated powders were densified into relative densities of 83–85% by high pressure CIPing (1 GPa). They were then presintered at 823 K for 3 min under uniaxial pressure of 100 MPa in Ar using a PECPS. The pre-sintered bodies had relative densities of 93–95% composed of spinel ferrite and permalloy; the mixed metal oxides were changed into magnesium ferrites by heating briefly at low temperature. Then, HIP (1123 K/6 h/196 MPa-Ar) was adopted to densify the pre-sintered bodies into a nearly full density; furthermore, a sintering atmosphere control was performed using ferrite muffles to maintain both phases. Sintered materials consisting of granular metal particles (φ 8.5 μm) isolated and surrounded by a thin ferrite discontinuous layer (0.2–1.3 μm) with a relative density ≥99.5% revealed both a saturation magnetization density ≥1 T and moderate permeability values of 30–35 at 1 MHz.</p></div>]]></content:encoded><description>Dense nanocomposites consisting of spinel Mn-doped Mg-ferrite and permalloy, (Mg[Fe1 − xMnx]2O4(0 ≤ x ≤ 0.4)/53Fe–47Ni), have been fabricated from powder mixtures of MgO/α-Fe2O3/MnO and N2-atomized metal particles utilizing high-pressure cold isostatic press (CIP), pulsed electric current pressure sintering (PECPS), and capsule-free hot isostatic pressing (HIP). Metal particles were coated with the mixed oxide powders homogeneously under high shear compression in Ar. The coated powders were densified into relative densities of 83–85% by high pressure CIPing (1 GPa). They were then presintered at 823 K for 3 min under uniaxial pressure of 100 MPa in Ar using a PECPS. The pre-sintered bodies had relative densities of 93–95% composed of spinel ferrite and permalloy; the mixed metal oxides were changed into magnesium ferrites by heating briefly at low temperature. Then, HIP (1123 K/6 h/196 MPa-Ar) was adopted to densify the pre-sintered bodies into a nearly full density; furthermore, a sintering atmosphere control was performed using ferrite muffles to maintain both phases. Sintered materials consisting of granular metal particles (φ 8.5 μm) isolated and surrounded by a thin ferrite discontinuous layer (0.2–1.3 μm) with a relative density ≥99.5% revealed both a saturation magnetization density ≥1 T and moderate permeability values of 30–35 at 1 MHz.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00710.x" xmlns="http://purl.org/rss/1.0/"><title>Tailoring the Relative Si3N4 and SiC Contents in Si3N4/SiC Nanopowders through Carbothermic Reduction and Nitridation of Silica Fume</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00710.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Tailoring the Relative Si3N4 and SiC Contents in Si3N4/SiC Nanopowders through Carbothermic Reduction and Nitridation of Silica Fume</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jyothi Suri, Leon L. Shaw, Mahmoud F. Zawrah</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-05T12:06:33.484411-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00710.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00710.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00710.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>This study demonstrates the synthesis of nanostructured Si<sub>3</sub>N<sub>4</sub>/SiC composite powders from silica fume, for the first time. The processing approach to convert the waste silica fume to advanced nanocomposites is based on the integrated mechanical and thermal activation (IMTA) process. The synthesized nanostructured <span class="fixed-roman">Si<sub>3</sub>N<sub>4</sub></span>/<span class="fixed-roman">SiC</span> powders have crystallite sizes as small as 17 nm for <span class="fixed-roman">SiC</span> and 42 nm for <span class="fixed-roman">Si<sub>3</sub>N<sub>4</sub></span>. It has been shown that the carbothermic reduction and nitridation temperature, as well as the graphite concentration in the starting <span class="fixed-roman">SiO<sub>2</sub></span> + <span class="fixed-roman">C</span> mixture are the important parameters to obtain <span class="fixed-roman">Si<sub>3</sub>N<sub>4</sub></span> and <span class="fixed-roman">SiC</span> nanopowders and control their crystal sizes. The synthesis conditions to tailor the relative contents of α-<span class="fixed-roman">Si<sub>3</sub>N<sub>4</sub></span> and α-<span class="fixed-roman">SiC</span> (changing from as high as 49 vol.% to as low as 21 vol.% α-<span class="fixed-roman">SiC</span>) in the final powder mixture have been investigated, and the mechanisms responsible for the observed relationship between processing conditions and the characteristics of the final powder have been identified.</p></div>]]></content:encoded><description>This study demonstrates the synthesis of nanostructured Si3N4/SiC composite powders from silica fume, for the first time. The processing approach to convert the waste silica fume to advanced nanocomposites is based on the integrated mechanical and thermal activation (IMTA) process. The synthesized nanostructured Si3N4/SiC powders have crystallite sizes as small as 17 nm for SiC and 42 nm for Si3N4. It has been shown that the carbothermic reduction and nitridation temperature, as well as the graphite concentration in the starting SiO2 + C mixture are the important parameters to obtain Si3N4 and SiC nanopowders and control their crystal sizes. The synthesis conditions to tailor the relative contents of α-Si3N4 and α-SiC (changing from as high as 49 vol.% to as low as 21 vol.% α-SiC) in the final powder mixture have been investigated, and the mechanisms responsible for the observed relationship between processing conditions and the characteristics of the final powder have been identified.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00708.x" xmlns="http://purl.org/rss/1.0/"><title>Synthesis of Ceramic Bonded Carbon Using SiC-Coated Carbon Particles and Spark Plasma Sintering</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00708.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Synthesis of Ceramic Bonded Carbon Using SiC-Coated Carbon Particles and Spark Plasma Sintering</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Masaharu Nakamura, Tetsuro Tojo, Makio Naito, Yoshinari Miyamoto</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-05T12:03:22.556345-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00708.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00708.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00708.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A dense SiC coating on carbon particles has been developed using SiO powders as the Si source and a chemical vapor reaction method. The coating process was controlled by atmosphere, coating temperature, time, and weight ratio of SiO/C. The SiC-coated carbon particles, with a mean particle size of 20 μm, were sintered at 2000°C under 40 MPa for 20 min by spark plasma sintering (SPS). The product, called ceramic bonded carbon (CBC), had a unique microstructure, with a 3D micro-network structure consisting of carbon particles covered with 1~5 μm thick SiC boundary layers. The sintering behavior of SiC/CBCs was analyzed in terms of the network formation of SiC boundary layers at over 1800°C and the grain growth of SiC at 2000°C. SiC/CBCs showed a bending strength of 150 MPa and a low shore hardness of 40. These materials could also be easily joined to SiC ceramics using SPS.</p></div>]]></content:encoded><description>A dense SiC coating on carbon particles has been developed using SiO powders as the Si source and a chemical vapor reaction method. The coating process was controlled by atmosphere, coating temperature, time, and weight ratio of SiO/C. The SiC-coated carbon particles, with a mean particle size of 20 μm, were sintered at 2000°C under 40 MPa for 20 min by spark plasma sintering (SPS). The product, called ceramic bonded carbon (CBC), had a unique microstructure, with a 3D micro-network structure consisting of carbon particles covered with 1~5 μm thick SiC boundary layers. The sintering behavior of SiC/CBCs was analyzed in terms of the network formation of SiC boundary layers at over 1800°C and the grain growth of SiC at 2000°C. SiC/CBCs showed a bending strength of 150 MPa and a low shore hardness of 40. These materials could also be easily joined to SiC ceramics using SPS.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00707.x" xmlns="http://purl.org/rss/1.0/"><title>Effect of Heating Schedule on Fabrication of Ti3SiC2-based Composites from Ti–SiC Powder Mixture</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00707.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of Heating Schedule on Fabrication of Ti3SiC2-based Composites from Ti–SiC Powder Mixture</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Pavel V. Istomin, Alexander V. Nadutkin, Vladislav E. Grass</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-05T11:59:27.485933-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00707.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00707.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00707.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>We herein describe a set of experiments used to study the effect of heating schedule on phase formation during the fabrication of <span class="fixed-roman">Ti<sub>3</sub>SiC<sub>2</sub></span>-based materials from <span class="fixed-roman">Ti–SiC</span> powder mixtures by means of pressureless sintering. We found that combustion was initiated at a temperature of about 1330°C, which resulted in the formation of <span class="fixed-roman">Ti</span>-rich eutectic melt followed by crystallization of <span class="fixed-roman">Ti<sub>3</sub>SiC<sub>2</sub></span>. It was shown that when preannealing was performed at 1150°C, no further combustive process could occur, and an intermediate, nonequilibrium phase composition, consisting of <span class="fixed-roman">Ti<sub>5</sub>Si<sub>3</sub>C</span><sub><em>x</em></sub>, <span class="fixed-roman">TiC</span>, and <span class="fixed-roman">SiC</span> remained until the end of the heat treatment. We herein discuss the mechanistic interpretation of this behavior.</p></div>]]></content:encoded><description>We herein describe a set of experiments used to study the effect of heating schedule on phase formation during the fabrication of Ti3SiC2-based materials from Ti–SiC powder mixtures by means of pressureless sintering. We found that combustion was initiated at a temperature of about 1330°C, which resulted in the formation of Ti-rich eutectic melt followed by crystallization of Ti3SiC2. It was shown that when preannealing was performed at 1150°C, no further combustive process could occur, and an intermediate, nonequilibrium phase composition, consisting of Ti5Si3Cx, TiC, and SiC remained until the end of the heat treatment. We herein discuss the mechanistic interpretation of this behavior.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00705.x" xmlns="http://purl.org/rss/1.0/"><title>Physicochemical Properties and Biocompatibility of White Dextrin Modified Injectable Calcium–Magnesium Phosphate Cement</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00705.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Physicochemical Properties and Biocompatibility of White Dextrin Modified Injectable Calcium–Magnesium Phosphate Cement</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Fangping Chen, Changsheng Liu, Jie Wei, Xiaolong Chen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-05T11:58:29.186453-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00705.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00705.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00705.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The objective of this study was to develop anti-washout and fast-setting calcium–magnesium phosphate cement (as-CMP) by introducing white dextrin (WD) and magnesium phosphate cement (MPC) to CPC. The results showed that WD imparted anti-washout to the as-CMP paste, whereas MPC simultaneously improved the paste anti-washout and fast-setting. The synergistic effect of MPC and WD obviously shortened the setting time of as-CMP. The WD did not affect the phase evolution and microstructure of the paste. Furthermore, all samples were biocompatible and as-CMP exhibited the best cell metabolic activity, cell attachment, and proliferation, which would provide basic data for the clinical application.</p></div>]]></content:encoded><description>The objective of this study was to develop anti-washout and fast-setting calcium–magnesium phosphate cement (as-CMP) by introducing white dextrin (WD) and magnesium phosphate cement (MPC) to CPC. The results showed that WD imparted anti-washout to the as-CMP paste, whereas MPC simultaneously improved the paste anti-washout and fast-setting. The synergistic effect of MPC and WD obviously shortened the setting time of as-CMP. The WD did not affect the phase evolution and microstructure of the paste. Furthermore, all samples were biocompatible and as-CMP exhibited the best cell metabolic activity, cell attachment, and proliferation, which would provide basic data for the clinical application.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00711.x" xmlns="http://purl.org/rss/1.0/"><title>Joining of Sintered Silicon Carbide Ceramics Using Sodium Borosilicate Glass as the Solder</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00711.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Joining of Sintered Silicon Carbide Ceramics Using Sodium Borosilicate Glass as the Solder</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Zhaohua Luo, Dongliang Jiang,, Jingxian Zhang, Qingling Lin, Zhongming Chen, Zhengren Huang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-05T11:56:27.863925-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00711.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00711.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00711.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Sodium borosilicate glass powder with the Si:B:Na molar ration of 53:44:6 has been developed and used as the solder to join sintered SiC ceramics. The coefficient of thermal expansion of the glass matches the silicon carbide substrate well at low temperature, and the wettability of the solder on SiC substrate becomes excellent above 1150°C. The 4-point bending strength of the joint reaches 218 ± 23 MPa at room temperature and the joint strength at 400°C can be kept at 154 ± 35 MPa. The microstructure, compositions, and interfacial properties were studied. Results showed that a good adhesion between SiC substrate and the solder layer was achieved.</p></div>]]></content:encoded><description>Sodium borosilicate glass powder with the Si:B:Na molar ration of 53:44:6 has been developed and used as the solder to join sintered SiC ceramics. The coefficient of thermal expansion of the glass matches the silicon carbide substrate well at low temperature, and the wettability of the solder on SiC substrate becomes excellent above 1150°C. The 4-point bending strength of the joint reaches 218 ± 23 MPa at room temperature and the joint strength at 400°C can be kept at 154 ± 35 MPa. The microstructure, compositions, and interfacial properties were studied. Results showed that a good adhesion between SiC substrate and the solder layer was achieved.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00696.x" xmlns="http://purl.org/rss/1.0/"><title>A Thermoanalytical Study of the Conversion of Amorphous Si–Ti–C–O Fibers to SiC</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00696.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A Thermoanalytical Study of the Conversion of Amorphous Si–Ti–C–O Fibers to SiC</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Nathan S. Jacobson, Sara E. Kline</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-02T10:47:34.890895-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00696.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00696.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00696.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The conversion of polytitanocarbosilane fibers to SiC has been studied from 1400°C to 1600°C. Thermochemical modeling indicated the stable phases were SiC and TiC. Kinetics were studied with a thermogravimetric method and post heat-treatment phases, and microstructures were studied with X-ray diffraction and scanning electron microscopy. Kinetics exhibit a strong temperature dependence and an activation energy of 443.3 ± 11.7 kJ/mol. This suggests that a chemical reaction step is rate-limiting. X-ray diffraction shows the conversion of an amorphous phase to crystalline SiC. Electron microscopy shows the development of internal porosity and large grains on the fiber surface, particularly at the higher temperatures.</p></div>]]></content:encoded><description>The conversion of polytitanocarbosilane fibers to SiC has been studied from 1400°C to 1600°C. Thermochemical modeling indicated the stable phases were SiC and TiC. Kinetics were studied with a thermogravimetric method and post heat-treatment phases, and microstructures were studied with X-ray diffraction and scanning electron microscopy. Kinetics exhibit a strong temperature dependence and an activation energy of 443.3 ± 11.7 kJ/mol. This suggests that a chemical reaction step is rate-limiting. X-ray diffraction shows the conversion of an amorphous phase to crystalline SiC. Electron microscopy shows the development of internal porosity and large grains on the fiber surface, particularly at the higher temperatures.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00697.x" xmlns="http://purl.org/rss/1.0/"><title>Effects and Control of Polymer-Converted Carbon Impurity in Synthesizing Continuous Boron Nitride Nanofibers by Electrospinning</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00697.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effects and Control of Polymer-Converted Carbon Impurity in Synthesizing Continuous Boron Nitride Nanofibers by Electrospinning</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yejun Qiu, Jie Yu, Jing Yin, Xiaosong Zhou</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-02T10:46:35.659951-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00697.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00697.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00697.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Application of polymer as thickener of precursor solution for preparing boron nitride (BN) nanofibers by electrospinning brings carbon impurity in the nitride products. The control and removal of the carbon impurity are a key step in the synthesis of the BN nanofibers. In this article, the control and removal of the carbon impurity are well realized by introducing O<sub>2</sub> and NH<sub>3</sub> simultaneously. The carbon content in the BN nanofibers can be well controlled by changing O<sub>2</sub>/NH<sub>3</sub> ratio, temperature, time, and gas flow rate. The effects of the carbon impurity on the structure of the BN products are investigated systematically.</p></div>]]></content:encoded><description>Application of polymer as thickener of precursor solution for preparing boron nitride (BN) nanofibers by electrospinning brings carbon impurity in the nitride products. The control and removal of the carbon impurity are a key step in the synthesis of the BN nanofibers. In this article, the control and removal of the carbon impurity are well realized by introducing O2 and NH3 simultaneously. The carbon content in the BN nanofibers can be well controlled by changing O2/NH3 ratio, temperature, time, and gas flow rate. The effects of the carbon impurity on the structure of the BN products are investigated systematically.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00695.x" xmlns="http://purl.org/rss/1.0/"><title>Benefits of the LTCC Substrate Configuration with an Air-Gap for Realization of RF Inductor with High Q-Factor and SRF</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00695.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Benefits of the LTCC Substrate Configuration with an Air-Gap for Realization of RF Inductor with High Q-Factor and SRF</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Goran J. Radosavljević, Andrea M. Marić, Walter Smetana, Ljiljana D. Živanov</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-02T10:43:00.52976-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00695.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00695.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00695.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>This article offers a detail description of design, simulation, fabrication and characterization of inductors on different substrate configurations intended for application in radio frequency range. The presented inductors are meander type structures fabricated using low temperature co-fired ceramic technology. Different substrate configurations incorporate placement of an air-gap beneath the inductor. Obtained results present over 30% increase in quality factor and widening of the operating frequency range by over 55% in comparison with inductors on standard substrate configurations.</p></div>]]></content:encoded><description>This article offers a detail description of design, simulation, fabrication and characterization of inductors on different substrate configurations intended for application in radio frequency range. The presented inductors are meander type structures fabricated using low temperature co-fired ceramic technology. Different substrate configurations incorporate placement of an air-gap beneath the inductor. Obtained results present over 30% increase in quality factor and widening of the operating frequency range by over 55% in comparison with inductors on standard substrate configurations.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00668.x" xmlns="http://purl.org/rss/1.0/"><title>(100) Three-Axis-Oriented BaTiO3, (Ba0.7Sr0.3)TiO3 Thin Film Prepared by Chemical Solution Deposition Method</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00668.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">(100) Three-Axis-Oriented BaTiO3, (Ba0.7Sr0.3)TiO3 Thin Film Prepared by Chemical Solution Deposition Method</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Tadasu Hosokura, Keisuke Kageyama, Hiroshi Takagi, Yukio Sakabe</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-11-23T11:28:25.308092-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00668.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00668.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00668.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Epitaxially grown (100) three-axis-oriented (Ba<sub>0.7</sub>Sr<sub>0.3</sub>)TiO<sub>3</sub> thin film on (100) platinum (Pt) coated (100) magnesium oxide (MgO) substrate and (100) three-axis-oriented BaTiO<sub>3</sub> thin film with BaZrO<sub>3</sub> buffer layer were prepared on an MgO(100) substrate using the chemical solution deposition method. The growth of the film was found to depend on the annealing condition. Transmission electron microscope revealed cube-on-cube epitaxial growth. The thin films exhibited a (100) three-axis-orientation that followed the (100) orientation of the MgO substrate and the (100) orientation of the Pt or BaZrO<sub>3</sub> bottom layer, as observed from an X-ray pole figure measurement and the selected area electron diffraction patterns.</p></div>]]></content:encoded><description>Epitaxially grown (100) three-axis-oriented (Ba0.7Sr0.3)TiO3 thin film on (100) platinum (Pt) coated (100) magnesium oxide (MgO) substrate and (100) three-axis-oriented BaTiO3 thin film with BaZrO3 buffer layer were prepared on an MgO(100) substrate using the chemical solution deposition method. The growth of the film was found to depend on the annealing condition. Transmission electron microscope revealed cube-on-cube epitaxial growth. The thin films exhibited a (100) three-axis-orientation that followed the (100) orientation of the MgO substrate and the (100) orientation of the Pt or BaZrO3 bottom layer, as observed from an X-ray pole figure measurement and the selected area electron diffraction patterns.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00675.x" xmlns="http://purl.org/rss/1.0/"><title>Ceramic Preforms with 2D Regular Channels for Fabrication of Metal/Ceramic-Reinforced Composites</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00675.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Ceramic Preforms with 2D Regular Channels for Fabrication of Metal/Ceramic-Reinforced Composites</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Osayande L. Ighodaro, Okenwa I. Okoli, Mei Zhang, Ben Wang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-31T11:20:32.513677-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00675.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00675.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00675.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Aligned regular 2D channels were fabricated in alumina via two routes: soft metal and carbon fibers. The soft metal route was accomplished employing centrifugal forces to eject the molten metal from the green matrix. The carbon fiber route was accomplished by burning out the carbon fibers between 450°C and 630°C. In both methods, pressureless sintering followed, yielding the desired 2D channel profiles. Some porous preforms exhibited higher fracture strength than the solid specimens, and this has been attributed to the ability of the channels to reduce the population and distribution of cracks in the porous material.</p></div>]]></content:encoded><description>Aligned regular 2D channels were fabricated in alumina via two routes: soft metal and carbon fibers. The soft metal route was accomplished employing centrifugal forces to eject the molten metal from the green matrix. The carbon fiber route was accomplished by burning out the carbon fibers between 450°C and 630°C. In both methods, pressureless sintering followed, yielding the desired 2D channel profiles. Some porous preforms exhibited higher fracture strength than the solid specimens, and this has been attributed to the ability of the channels to reduce the population and distribution of cracks in the porous material.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00691.x" xmlns="http://purl.org/rss/1.0/"><title>Effect of Pore Characteristics in Slip Cast Alumina on Glass Infiltration and Mechanical Properties of the Composites</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00691.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of Pore Characteristics in Slip Cast Alumina on Glass Infiltration and Mechanical Properties of the Composites</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Preeti Bajpai, Parag Bhargava</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-24T10:09:30.897033-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00691.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00691.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00691.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Development of alumina/glass composites with minimal residual porosity and superior mechanical properties requires systematic studies on glass infiltration into porous alumina. This work has examined the effect of alumina particle size and the resulting pore size distribution on glass infiltration. Samples were prepared by slip-casting a coarser alumina powder and blends of the coarse (<em>d</em><sub>50</sub> ~ 3.4 μm) and a finer (<em>d</em><sub>50</sub> ~ 0.7 μm) alumina powder. After presintering (1200°C) and following a single cycle of infiltration (1100°C), the sample with 50:50 (wt%) coarse and fine alumina showed highest flexural strength. Improvement in flexural strength could be imputed to the better glass infiltration.</p></div>]]></content:encoded><description>Development of alumina/glass composites with minimal residual porosity and superior mechanical properties requires systematic studies on glass infiltration into porous alumina. This work has examined the effect of alumina particle size and the resulting pore size distribution on glass infiltration. Samples were prepared by slip-casting a coarser alumina powder and blends of the coarse (d50 ~ 3.4 μm) and a finer (d50 ~ 0.7 μm) alumina powder. After presintering (1200°C) and following a single cycle of infiltration (1100°C), the sample with 50:50 (wt%) coarse and fine alumina showed highest flexural strength. Improvement in flexural strength could be imputed to the better glass infiltration.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00704.x" xmlns="http://purl.org/rss/1.0/"><title>CoAl2O4 Nano Pigment Obtained by Combustion Synthesis</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00704.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">CoAl2O4 Nano Pigment Obtained by Combustion Synthesis</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Shiva Salem, Seyed Hamid Jazayeri, Federica Bondioli, Ali Allahverdi, Mansoor Shirvani, Anna Maria Ferrari</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-24T10:02:08.54695-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00704.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00704.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00704.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The aim of this research was to study the influence of pH (2.5, 7, 10.5), molar ratio of fuel to nitrates (0.36, 0.56, 0.75), and calcination temperature (600, 800, 1000, 1200°C) on the characteristics of CoAl<sub>2</sub>O<sub>4</sub> nano pigments synthesized using a solution-based combustion method. Gel formation, morphology, specific surface area, and color of the powder were characterized using TG–DTA (thermogravimetric and differential thermal analysis), XRD (X-ray diffraction), TEM (transmission electron microscopy), BET (Brunauer–Emmett–Teller), and UV–Vis. The results indicate that spinel CoAl<sub>2</sub>O<sub>4</sub> was formed independently of the different variables studied and that higher temperature promotes crystallite size. According to the TEM micrographs, most of particles calcined at 800 and 1000°C have average particle sizes &lt;30 and 75 nm, respectively. Consistent with BET results, maximum specific surface area was obtained at pH of 7. Colorability tests demonstrate that the mixtures of glaze and calcined nano pigments are still dark blue after heating up to 1200°C.</p></div>]]></content:encoded><description>The aim of this research was to study the influence of pH (2.5, 7, 10.5), molar ratio of fuel to nitrates (0.36, 0.56, 0.75), and calcination temperature (600, 800, 1000, 1200°C) on the characteristics of CoAl2O4 nano pigments synthesized using a solution-based combustion method. Gel formation, morphology, specific surface area, and color of the powder were characterized using TG–DTA (thermogravimetric and differential thermal analysis), XRD (X-ray diffraction), TEM (transmission electron microscopy), BET (Brunauer–Emmett–Teller), and UV–Vis. The results indicate that spinel CoAl2O4 was formed independently of the different variables studied and that higher temperature promotes crystallite size. According to the TEM micrographs, most of particles calcined at 800 and 1000°C have average particle sizes &lt;30 and 75 nm, respectively. Consistent with BET results, maximum specific surface area was obtained at pH of 7. Colorability tests demonstrate that the mixtures of glaze and calcined nano pigments are still dark blue after heating up to 1200°C.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00703.x" xmlns="http://purl.org/rss/1.0/"><title>Microstructure Contact Studies for Skutterudite Thermoelectric Devices</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00703.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Microstructure Contact Studies for Skutterudite Thermoelectric Devices</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Degang Zhao, Haoran Geng, Lidong Chen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-24T10:01:48.608071-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00703.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00703.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00703.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The skutterudite/electrode thermoelectric joints were fabricated with the insertion of Ti foil by spark plasma sintering. The interfacial microstructure and reliability of joints were studied during thermal duration test. A multilayer structure, which was composed of intermetallic compounds, was observed at the CoSb<sub>3</sub>/Ti interface after thermal aging of 20 days. The interfacial reactions and diffusion path between CoSb<sub>3</sub> and Ti were discussed. The contact resistance of CoSb<sub>3</sub>/electrode junction was measured through four-probe method and the thermal contact resistance was calculated based on multilayer mode measurement. Effects of the contact resistivity on the performance of CoSb<sub>3</sub>-based device were discussed.</p></div>]]></content:encoded><description>The skutterudite/electrode thermoelectric joints were fabricated with the insertion of Ti foil by spark plasma sintering. The interfacial microstructure and reliability of joints were studied during thermal duration test. A multilayer structure, which was composed of intermetallic compounds, was observed at the CoSb3/Ti interface after thermal aging of 20 days. The interfacial reactions and diffusion path between CoSb3 and Ti were discussed. The contact resistance of CoSb3/electrode junction was measured through four-probe method and the thermal contact resistance was calculated based on multilayer mode measurement. Effects of the contact resistivity on the performance of CoSb3-based device were discussed.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00702.x" xmlns="http://purl.org/rss/1.0/"><title>Two-Step Sintering of Pristine and Aluminum-Doped Zinc Oxide Ceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00702.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Two-Step Sintering of Pristine and Aluminum-Doped Zinc Oxide Ceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yulong Zhang, Ruiqin Tan, Ye Yang, Xianpeng Zhang, Weiyan Wang, Ping Cui, Weijie Song</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-24T10:01:37.922985-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00702.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00702.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00702.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p><span class="fixed-roman">ZnO</span> and <span class="fixed-roman">Al</span>-doped <span class="fixed-roman">ZnO</span> ceramics with high density and fine grain size were prepared using a two-step sintering method. <span class="fixed-roman">ZnO</span> ceramics with a grain size of 1.2 μm and a density greater than 99% were obtained. The kinetic window for a <span class="fixed-roman">ZnO</span> nanoparticle TSS process was determined in this study. Dense AZO ceramics with homogeneous <span class="fixed-roman">Al</span> distribution were obtained using a high sintering temperature (<em>T</em><sub>st</sub>) of 1323 K and a low sintering temperature (<em>T</em><sub>nd</sub>) of 1273 K. The activation energies for <span class="fixed-roman">ZnO</span> and AZO nanoparticle grain growth were determined to be 169 ± 18 kJ/mol and 374 ± 36 kJ/mol, respectively.</p></div>]]></content:encoded><description>ZnO and Al-doped ZnO ceramics with high density and fine grain size were prepared using a two-step sintering method. ZnO ceramics with a grain size of 1.2 μm and a density greater than 99% were obtained. The kinetic window for a ZnO nanoparticle TSS process was determined in this study. Dense AZO ceramics with homogeneous Al distribution were obtained using a high sintering temperature (Tst) of 1323 K and a low sintering temperature (Tnd) of 1273 K. The activation energies for ZnO and AZO nanoparticle grain growth were determined to be 169 ± 18 kJ/mol and 374 ± 36 kJ/mol, respectively.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00701.x" xmlns="http://purl.org/rss/1.0/"><title>The Influence of Cavity-defect Shapes on Resonant Peak of Three-dimensional Electromagnetic Band Gap Structure</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00701.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">The Influence of Cavity-defect Shapes on Resonant Peak of Three-dimensional Electromagnetic Band Gap Structure</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Shibin Chen, Dichen Li, Haoxue Han, Gai Yang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-24T10:01:24.648516-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00701.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00701.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00701.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Localized mode is an important property of defect electromagnetic band gap (EBG) structure, which plays a key role in the application of EBG structure. The purpose of this article was to study the impact on localized properties by introducing cavities of different shapes into diamond EBG structure. Alumina-based ceramic diamond EBG structures were fabricated using stereolithography (SL), gel-casting and vacuum freeze-drying. When the microwave transmission properties of samples with cavities of different shapes were tested, the resonant peaks appeared within the band gap. By varying the cavity shape, the quality of the localized mode could be adjusted. The results have shown that localized mode with a high quality factor (<em>Q</em> factor) corresponded to the optimal cavity shape in EBG structure. The experimental results agreed well with simulation results. These excellent microwave properties of 3D EBG structure could be directly applied in microwave devices, such as microwave antenna and filter devices.</p></div>]]></content:encoded><description>Localized mode is an important property of defect electromagnetic band gap (EBG) structure, which plays a key role in the application of EBG structure. The purpose of this article was to study the impact on localized properties by introducing cavities of different shapes into diamond EBG structure. Alumina-based ceramic diamond EBG structures were fabricated using stereolithography (SL), gel-casting and vacuum freeze-drying. When the microwave transmission properties of samples with cavities of different shapes were tested, the resonant peaks appeared within the band gap. By varying the cavity shape, the quality of the localized mode could be adjusted. The results have shown that localized mode with a high quality factor (Q factor) corresponded to the optimal cavity shape in EBG structure. The experimental results agreed well with simulation results. These excellent microwave properties of 3D EBG structure could be directly applied in microwave devices, such as microwave antenna and filter devices.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00693.x" xmlns="http://purl.org/rss/1.0/"><title>Electrical Properties of Pb0.92La0.08Zr0.52Ti0.48O3 Thin Films Grown on SrRuO3 Buffered Nickel and Silicon Substrates by Chemical Solution Deposition</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00693.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Electrical Properties of Pb0.92La0.08Zr0.52Ti0.48O3 Thin Films Grown on SrRuO3 Buffered Nickel and Silicon Substrates by Chemical Solution Deposition</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Manoj Narayanan, Beihai Ma, Sheng Tong, Rachel Koritala, Uthamalingam Balachandran</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-24T10:00:42.945468-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00693.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00693.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00693.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Ferroelectric film-on-foil capacitors are suitable to replace discrete passive components in the quest to develop electronic devices that show superior performance and are smaller in size. The film-on-foil approach is the most practical method to fabricate such components. Films of Pb<sub>0.92</sub>La<sub>0.08</sub>Zr<sub>0.52</sub>Ti<sub>0.48</sub>O<sub>3</sub> (PLZT) were deposited on SrRuO<sub>3</sub> (SRO) buffer films over nickel and silicon substrates. High-quality polycrystalline SRO thin-film electrodes were first deposited by chemical solution deposition. A phase pure, dense, uniform microstructure with grain size &lt;100 nm was obtained in films crystallized at 700°C. The room-temperature resistivity of the SRO films crystallized at 700°C was ~800–900 μΩ-cm. The dielectric properties of sol–gel derived PLZT capacitors on SRO-buffered nickel were evaluated as a function of temperature, bias field, and frequency, and the results were compared to those of the same films on silicon substrates. The comparison demonstrated the integrity of the buffer layer and its compatibility with nickel substrates. Device-quality dielectric properties were measured on PLZT films deposited on SRO-buffered nickel foils and found to be superior to those for PLZT on SRO-buffered silicon and expensive platinized silicon. These results suggest that SRO films can act as an effective barrier layer on nickel substrates suitable for embedded capacitor applications.</p></div>]]></content:encoded><description>Ferroelectric film-on-foil capacitors are suitable to replace discrete passive components in the quest to develop electronic devices that show superior performance and are smaller in size. The film-on-foil approach is the most practical method to fabricate such components. Films of Pb0.92La0.08Zr0.52Ti0.48O3 (PLZT) were deposited on SrRuO3 (SRO) buffer films over nickel and silicon substrates. High-quality polycrystalline SRO thin-film electrodes were first deposited by chemical solution deposition. A phase pure, dense, uniform microstructure with grain size &lt;100 nm was obtained in films crystallized at 700°C. The room-temperature resistivity of the SRO films crystallized at 700°C was ~800–900 μΩ-cm. The dielectric properties of sol–gel derived PLZT capacitors on SRO-buffered nickel were evaluated as a function of temperature, bias field, and frequency, and the results were compared to those of the same films on silicon substrates. The comparison demonstrated the integrity of the buffer layer and its compatibility with nickel substrates. Device-quality dielectric properties were measured on PLZT films deposited on SRO-buffered nickel foils and found to be superior to those for PLZT on SRO-buffered silicon and expensive platinized silicon. These results suggest that SRO films can act as an effective barrier layer on nickel substrates suitable for embedded capacitor applications.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00692.x" xmlns="http://purl.org/rss/1.0/"><title>Effect of ZrO2 (YPSZ) on Microstructure Characteristic and Wear Resistance of the Ti3Al/TiC Laser-Cladded Ceramic Layer on Titanium Alloy</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00692.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of ZrO2 (YPSZ) on Microstructure Characteristic and Wear Resistance of the Ti3Al/TiC Laser-Cladded Ceramic Layer on Titanium Alloy</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Li Jianing, Chen Chuanzhong</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-24T10:00:27.10296-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00692.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00692.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00692.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Laser cladding of the <span class="fixed-roman">A<sub>3</sub>Ti + TiC</span> preplaced powders on the <span class="fixed-roman">Ti–6Al–4V</span> alloy can form the <span class="fixed-roman">Ti<sub>3</sub>Al/TiC</span> ceramic layer, which improved the wear resistance of the substrate. In this study, the influence of 7 wt% yttria partially stabilized zirconia (YPSZ) on the surface performance of the <span class="fixed-roman">Ti<sub>3</sub>Al/TiC</span> ceramic layer was researched, and the <span class="fixed-roman">Al<sub>3</sub>Ti + TiC</span>/YPSZ laser-cladded coating has been researched by means of X-ray diffraction, scanning electron microscope, and energy dispersive spectrometer. It was found that laser cladding of YPSZ can control the cracks in the <span class="fixed-roman">Ti<sub>3</sub>Al/TiC</span> ceramic layer. Furthermore, due to the action of YPSZ, stratification was observed in this ceramic layer. The upper layer in this coating consisted of <span class="fixed-roman">Al<sub>2</sub>O<sub>3,</sub> Ti<sub>3</sub>Al</span>, <em>t</em>-<span class="fixed-roman">ZrO<sub>2</sub>, TiC, TiO<sub>2</sub></span> and <span class="fixed-roman">ZrSiO<sub>4</sub></span>, and <span class="fixed-roman">Ti<sub>3</sub>Al/Al<sub>2</sub>O<sub>3</sub></span> were the matrix of this region. This upper layer exhibited an excellent wear resistance due to its phase constituent. During the cladding process, YPSZ had a very marked trend to float on the surface of the coating. Therefore, the upper layer showed better wear resistance than that of the bottom layer due to the action of the high YPSZ content.</p></div>]]></content:encoded><description>Laser cladding of the A3Ti + TiC preplaced powders on the Ti–6Al–4V alloy can form the Ti3Al/TiC ceramic layer, which improved the wear resistance of the substrate. In this study, the influence of 7 wt% yttria partially stabilized zirconia (YPSZ) on the surface performance of the Ti3Al/TiC ceramic layer was researched, and the Al3Ti + TiC/YPSZ laser-cladded coating has been researched by means of X-ray diffraction, scanning electron microscope, and energy dispersive spectrometer. It was found that laser cladding of YPSZ can control the cracks in the Ti3Al/TiC ceramic layer. Furthermore, due to the action of YPSZ, stratification was observed in this ceramic layer. The upper layer in this coating consisted of Al2O3, Ti3Al, t-ZrO2, TiC, TiO2 and ZrSiO4, and Ti3Al/Al2O3 were the matrix of this region. This upper layer exhibited an excellent wear resistance due to its phase constituent. During the cladding process, YPSZ had a very marked trend to float on the surface of the coating. Therefore, the upper layer showed better wear resistance than that of the bottom layer due to the action of the high YPSZ content.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00690.x" xmlns="http://purl.org/rss/1.0/"><title>Lifetime and Wear Behavior of Near Net Shaped Si3N4/SiC Wood Cutting Tools</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00690.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Lifetime and Wear Behavior of Near Net Shaped Si3N4/SiC Wood Cutting Tools</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Claudia Strehler, Bruno Ehrle, Andreas Weinreich, Benjamin Kaiser, Thomas Graule, Christos G. Aneziris, Jakob Kuebler</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-24T09:59:47.745649-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00690.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00690.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00690.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The introduction of ceramics into the market of wood cutting tools has been difficult because of the generally low toughness of ceramics which causes brittle failure. That is why the improvement of mechanical performance of ceramics with potential to be used as cutting tools is important. The newly developed <span class="fixed-roman">Si<sub>3</sub>N<sub>4</sub>/SiC</span> wood cutting tools have a bending strength of 740 MPa, a fracture toughness of 5.4 MPam<sup>1/2</sup>, a hardness of 16.8 GPa and a grain size of 1 μm. These <span class="fixed-roman">Si<sub>3</sub>N<sub>4</sub>/SiC</span> tools were tested in a lifetime cutting trial on wood and showed twice as long lifecycles than standard tungsten carbide tools. Furthermore, the static corrosion resistance in tannic acid, the friction coefficients between wood and the tool material and the cutting forces were measured for both the ceramic composite and the tungsten carbide tools.</p></div>]]></content:encoded><description>The introduction of ceramics into the market of wood cutting tools has been difficult because of the generally low toughness of ceramics which causes brittle failure. That is why the improvement of mechanical performance of ceramics with potential to be used as cutting tools is important. The newly developed Si3N4/SiC wood cutting tools have a bending strength of 740 MPa, a fracture toughness of 5.4 MPam1/2, a hardness of 16.8 GPa and a grain size of 1 μm. These Si3N4/SiC tools were tested in a lifetime cutting trial on wood and showed twice as long lifecycles than standard tungsten carbide tools. Furthermore, the static corrosion resistance in tannic acid, the friction coefficients between wood and the tool material and the cutting forces were measured for both the ceramic composite and the tungsten carbide tools.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00688.x" xmlns="http://purl.org/rss/1.0/"><title>Silicon Volatility From Alumina and Aluminosilicates Under Solid Oxide Fuel Cell Operating Conditions</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00688.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Silicon Volatility From Alumina and Aluminosilicates Under Solid Oxide Fuel Cell Operating Conditions</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Paul S. Gentile, Stephen W. Sofie, Camas F. Key, Richard J. Smith</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-24T09:59:29.732629-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00688.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00688.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00688.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Thermodynamic equilibrium modeling indicates that the introduction of H<sub>2</sub>O in oxidizing environments decreases Si stability due to formation of volatile hydroxide and oxy hydroxides. 3Al<sub>2</sub>O<sub>3</sub>·2SiO<sub>2</sub> mullite bond offers only slight improvement over pure silica as the thermodynamic activity of silica in mullite is near unity. In reducing atmospheres Si stability is improved by the presence of H<sub>2</sub>O and Al<sub>2</sub>O<sub>3</sub>, transitioning from SiO and silane as the dominant volatile species to hydroxides, oxy hydroxides, and SiO with increasing water vapor partial pressure. Empirical studies reveal initial rapid releases of Si from stationary solid oxide fuel cell refractory materials followed by slower solid-state diffusion limited release.</p></div>]]></content:encoded><description>Thermodynamic equilibrium modeling indicates that the introduction of H2O in oxidizing environments decreases Si stability due to formation of volatile hydroxide and oxy hydroxides. 3Al2O3·2SiO2 mullite bond offers only slight improvement over pure silica as the thermodynamic activity of silica in mullite is near unity. In reducing atmospheres Si stability is improved by the presence of H2O and Al2O3, transitioning from SiO and silane as the dominant volatile species to hydroxides, oxy hydroxides, and SiO with increasing water vapor partial pressure. Empirical studies reveal initial rapid releases of Si from stationary solid oxide fuel cell refractory materials followed by slower solid-state diffusion limited release.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00686.x" xmlns="http://purl.org/rss/1.0/"><title>Knoop Hardness–Apparent Yield Stress Relationship in Ceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00686.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Knoop Hardness–Apparent Yield Stress Relationship in Ceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jeffrey J. Swab, Andrew A. Wereszczak, Kevin T. Strong, Dominic Danna, Jerry C. LaSalvia, Meredith E. Ragan, Patrick J. Ritt</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-24T09:59:00.55594-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00686.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00686.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00686.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>In Tabor's classical studies of the deformation of metals, the yield stress (<em>Y</em>) and hardness (<em>H</em>) were shown to be related according to <em>H</em>/<em>Y</em> ≈ 3 for complete or fully plastic deformation. Since then it has been anecdotally shown for ceramics that this ratio is &lt;3. Interest exists to explore this further so Hertzian indentation was used to measure the apparent yield stress of numerous ceramics and metals and their results were compared with each material's load-dependent Knoop hardness. The evaluated ceramics included standard reference materials for hardness (silicon nitride and tungsten carbide), silicon carbide, alumina, and glass. Several steel compositions were also tested for comparison. Knoop hardness measurements at 19.6 N (i.e., toward “complete or fully plastic deformation”), showed that 2 &lt; <em>H</em>/<em>Y</em> &lt; 3 for the metals and 0.8 &lt; <em>H</em>/<em>Y</em> &lt; 1.8 for the glasses and ceramics. Being that <em>H</em>/<em>Y</em> ≠ 3 for the ceramics indicates that Tabor's analysis is either not applicable to ceramics or that full plastic deformation is not achieved with a Knoop indentation or both.</p></div>]]></content:encoded><description>In Tabor's classical studies of the deformation of metals, the yield stress (Y) and hardness (H) were shown to be related according to H/Y ≈ 3 for complete or fully plastic deformation. Since then it has been anecdotally shown for ceramics that this ratio is &lt;3. Interest exists to explore this further so Hertzian indentation was used to measure the apparent yield stress of numerous ceramics and metals and their results were compared with each material's load-dependent Knoop hardness. The evaluated ceramics included standard reference materials for hardness (silicon nitride and tungsten carbide), silicon carbide, alumina, and glass. Several steel compositions were also tested for comparison. Knoop hardness measurements at 19.6 N (i.e., toward “complete or fully plastic deformation”), showed that 2 &lt; H/Y &lt; 3 for the metals and 0.8 &lt; H/Y &lt; 1.8 for the glasses and ceramics. Being that H/Y ≠ 3 for the ceramics indicates that Tabor's analysis is either not applicable to ceramics or that full plastic deformation is not achieved with a Knoop indentation or both.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00685.x" xmlns="http://purl.org/rss/1.0/"><title>A Prospective Way to Reduce Emissions in Secondary Steel Making Metallurgy by Application of Functionalized Doloma Carbon Refractories</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00685.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A Prospective Way to Reduce Emissions in Secondary Steel Making Metallurgy by Application of Functionalized Doloma Carbon Refractories</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Volker Stein, Christos G. Aneziris, Erwan Guéguen, Keith Hill</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-21T12:12:05.653362-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00685.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00685.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00685.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Doloma and doloma carbon refractories are the standard refractory systems applied in AOD (argon oxygen decarburization) and VOD (vacuum oxygen decarburization) vessels in the secondary metallurgy to produce stainless steel. This refractory system is connected with metallurgical benefits such as high oxidic stability of its oxides, and the ability to bond sulfur from the hot metal. Production and application of carbon-bonded refractories is directly linked with environmental harmful emissions in the broadest sense. In the center of this work is the aspect of increased residual carbon content of the binder resin due to TiO<sub>2</sub> addition. Furthermore, this work has observed the applicability of TiO<sub>2</sub>-treated bricks in AOD converter. The increased residual carbon content of the binder resin connected with improved mechanical, physical, and thermomechanical properties due to sub-micro scaled TiO<sub>2</sub> and metallic antioxidant addition offers the feasibility to reduce the total carbon content without downgrading the brick properties. This aspect has not been observed yet, and is of high interest with respect to reduced emissions and environmental friendly refractories. Previous works have investigated the influence of TiO<sub>2</sub> on other carbon-bonded refractory systems, such as alumina carbon and magnesia carbon. As illustrated in this work and previous work, TiO<sub>2</sub> is working completely different in the doloma carbon system when compared with other systems.</p></div>]]></content:encoded><description>Doloma and doloma carbon refractories are the standard refractory systems applied in AOD (argon oxygen decarburization) and VOD (vacuum oxygen decarburization) vessels in the secondary metallurgy to produce stainless steel. This refractory system is connected with metallurgical benefits such as high oxidic stability of its oxides, and the ability to bond sulfur from the hot metal. Production and application of carbon-bonded refractories is directly linked with environmental harmful emissions in the broadest sense. In the center of this work is the aspect of increased residual carbon content of the binder resin due to TiO2 addition. Furthermore, this work has observed the applicability of TiO2-treated bricks in AOD converter. The increased residual carbon content of the binder resin connected with improved mechanical, physical, and thermomechanical properties due to sub-micro scaled TiO2 and metallic antioxidant addition offers the feasibility to reduce the total carbon content without downgrading the brick properties. This aspect has not been observed yet, and is of high interest with respect to reduced emissions and environmental friendly refractories. Previous works have investigated the influence of TiO2 on other carbon-bonded refractory systems, such as alumina carbon and magnesia carbon. As illustrated in this work and previous work, TiO2 is working completely different in the doloma carbon system when compared with other systems.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00684.x" xmlns="http://purl.org/rss/1.0/"><title>Low Temperature Sintering and Dielectric Properties of Alumina-Filled Glass Composites for LTCC Applications</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00684.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Low Temperature Sintering and Dielectric Properties of Alumina-Filled Glass Composites for LTCC Applications</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Surendran Rajesh, Heli Jantunen, Martin Letz, Sabine Pichler-Willhelm</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-21T12:11:55.664404-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00684.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00684.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00684.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Glass + ceramic composites using lead-free ultralow-softening point glass matrices (brand names G018-249 and G018-250) with alumina fillers are investigated. The composites show good densification with near zero shrinkage at very low sintering temperature and do not show either the formation of secondary crystalline phases or dissolution of alumina. They further show no reactivity with the silver electrodes at a sintering temperature of 650°C and have permittivities of 9.5 and 8.8, loss tangents of 0.0068 and 0.0087 at 1 MHz for the samples containing G018-249 glass and G018-250 glass, respectively.</p></div>]]></content:encoded><description>Glass + ceramic composites using lead-free ultralow-softening point glass matrices (brand names G018-249 and G018-250) with alumina fillers are investigated. The composites show good densification with near zero shrinkage at very low sintering temperature and do not show either the formation of secondary crystalline phases or dissolution of alumina. They further show no reactivity with the silver electrodes at a sintering temperature of 650°C and have permittivities of 9.5 and 8.8, loss tangents of 0.0068 and 0.0087 at 1 MHz for the samples containing G018-249 glass and G018-250 glass, respectively.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00683.x" xmlns="http://purl.org/rss/1.0/"><title>Improved Microwave Dielectric Properties of La(Mg0.5Sn0.5)O3 Ceramics with Yb3+ Doping</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00683.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Improved Microwave Dielectric Properties of La(Mg0.5Sn0.5)O3 Ceramics with Yb3+ Doping</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yih-Chien Chen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-21T12:11:44.910482-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00683.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00683.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00683.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The <span class="fixed-roman">La<sub>1−<em>x</em></sub>Yb<sub><em>x</em></sub>(Mg<sub>0.5</sub>Sn<sub>0.5</sub>)O<sub>3</sub></span> ceramics were prepared by the conventional solid-state method with various sintering temperatures. The X-ray diffraction patterns of the <span class="fixed-roman">La<sub>0.97</sub>Yb<sub>0.03</sub>(Mg<sub>0.5</sub>Sn<sub>0.5</sub>)O<sub>3</sub></span> ceramics revealed no significant variation of phase with sintering temperatures. An apparent density of 6.65 g/cm<sup>3</sup>, a dielectric constant (<em>ε</em><sub>r</sub>) of 20.2, a quality factor (<em>Q</em> × <em>f</em>) of 56,800 GHz, and a temperature coefficient of resonant frequency (<em>τ</em><sub><em>f</em></sub>) of −76.9 ppm/°C were obtained for <span class="fixed-roman">La<sub>0.97</sub>Yb<sub>0.03</sub>(Mg<sub>0.5</sub>Sn<sub>0.5</sub>)O<sub>3</sub></span> ceramics that were sintered at 1550°C for 4 h.</p></div>]]></content:encoded><description>The La1−xYbx(Mg0.5Sn0.5)O3 ceramics were prepared by the conventional solid-state method with various sintering temperatures. The X-ray diffraction patterns of the La0.97Yb0.03(Mg0.5Sn0.5)O3 ceramics revealed no significant variation of phase with sintering temperatures. An apparent density of 6.65 g/cm3, a dielectric constant (εr) of 20.2, a quality factor (Q × f) of 56,800 GHz, and a temperature coefficient of resonant frequency (τf) of −76.9 ppm/°C were obtained for La0.97Yb0.03(Mg0.5Sn0.5)O3 ceramics that were sintered at 1550°C for 4 h.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00682.x" xmlns="http://purl.org/rss/1.0/"><title>Influence of Sintering Temperature on the Mechanical Properties of Alumina Springs</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00682.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Influence of Sintering Temperature on the Mechanical Properties of Alumina Springs</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Rodrigo A. Barbieri, Cláudio A. Perottoni, Janete E. Zorzi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-21T12:11:32.715851-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00682.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00682.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00682.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Low-pressure injection molding (LPIM) was used to produce helical alumina springs. Three sets of springs were sintered at 1550°C, 1600°C and 1650°C to observe the effects on spring constant and fracture stress. Sintered alumina springs were obtained with densities ranging from 94.0% to 97.5% of the theoretical limit. Spring constants were measured from room temperature up to 1100°C. Fracture stress data were analyzed according to Weibull statistics and the method of maximum likelihood. Upon increase of sintering temperature from 1550°C to 1650°C, the spring constant and the Weibull characteristic strength of the alumina springs increases by 15% and 32%, respectively. On the other hand, sintering temperature has a negligible influence on Weibull's modulus. This is because internal bubbles and surface defects introduced in the production stage of the ceramic springs — more than the reduction in porosity with increasing sintering temperature — are critical in determining the reliability of the ceramic springs.</p></div>]]></content:encoded><description>Low-pressure injection molding (LPIM) was used to produce helical alumina springs. Three sets of springs were sintered at 1550°C, 1600°C and 1650°C to observe the effects on spring constant and fracture stress. Sintered alumina springs were obtained with densities ranging from 94.0% to 97.5% of the theoretical limit. Spring constants were measured from room temperature up to 1100°C. Fracture stress data were analyzed according to Weibull statistics and the method of maximum likelihood. Upon increase of sintering temperature from 1550°C to 1650°C, the spring constant and the Weibull characteristic strength of the alumina springs increases by 15% and 32%, respectively. On the other hand, sintering temperature has a negligible influence on Weibull's modulus. This is because internal bubbles and surface defects introduced in the production stage of the ceramic springs — more than the reduction in porosity with increasing sintering temperature — are critical in determining the reliability of the ceramic springs.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00681.x" xmlns="http://purl.org/rss/1.0/"><title>Solution Precursor Plasma Spray Eu: Y2O3 Phosphor Coating</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00681.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Solution Precursor Plasma Spray Eu: Y2O3 Phosphor Coating</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dianying Chen, Eric H. Jordan, Michael W. Renfro, Maurice Gell</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-21T12:11:24.285306-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00681.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00681.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00681.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Using the solution precursor plasma spray process <span class="fixed-roman">Eu</span>: <span class="fixed-roman">Y<sub>2</sub>O<sub>3</sub></span> phosphor coating was deposited. The phase composition, microstructure, and photoluminescent properties of the as-synthesized powders and as-deposited coatings were investigated. XRD analysis indicated that the coating is composed of cubic <span class="fixed-roman">Y<sub>2</sub>O<sub>3</sub></span>. SEM micrographs reveal the as-sprayed coating is porous with a thickness of ~150 μm. Photoluminescent property measurement indicated that the phosphor coating exhibits the strongest emission at 612 nm, which is assigned to <span class="fixed-roman"><sup>5</sup>D<sub>0</sub></span> → <span class="fixed-roman"><sup>7</sup>F<sub>2</sub></span> electric-dipole transition.</p></div>]]></content:encoded><description>Using the solution precursor plasma spray process Eu: Y2O3 phosphor coating was deposited. The phase composition, microstructure, and photoluminescent properties of the as-synthesized powders and as-deposited coatings were investigated. XRD analysis indicated that the coating is composed of cubic Y2O3. SEM micrographs reveal the as-sprayed coating is porous with a thickness of ~150 μm. Photoluminescent property measurement indicated that the phosphor coating exhibits the strongest emission at 612 nm, which is assigned to 5D0 → 7F2 electric-dipole transition.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00679.x" xmlns="http://purl.org/rss/1.0/"><title>The Production of Transparent MgAl2O4 Ceramic Using Calcined Powder Mixtures of Mg(OH)2 and γ-Al2O3 or AlOOH</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00679.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">The Production of Transparent MgAl2O4 Ceramic Using Calcined Powder Mixtures of Mg(OH)2 and γ-Al2O3 or AlOOH</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Anthony C. Sutorik, Gary Gilde, Jeffrey J. Swab, Christopher Cooper, Robert Gamble, Eugene Shanholtz</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-21T12:11:18.824642-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00679.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00679.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00679.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Magnesium hydroxide, Mg(OH)<sub>2</sub> (both 99% and 99.99% purity grades), γ-Al<sub>2</sub>O<sub>3</sub>, and AlOOH have been investigated for the direct production of transparent MgAl<sub>2</sub>O<sub>4</sub>. The highest average in-line transmittance through 3.5–4 mm thick samples is 84.2 ± 1.0% at 550 nm, attained by using mixtures of 99.99% pure Mg(OH)<sub>2</sub> and γ-Al<sub>2</sub>O<sub>3</sub>. Other formulations exhibited 77–80% visible transmission, suggesting that further optimization can improve sample consistency. All samples exhibited a Knoop hardness of ~12 GPa, and elastic modulus of ~280 GPa. Biaxial flexural strength measurements ranged from 85 to 136 MPa depending on starting materials.</p></div>]]></content:encoded><description>Magnesium hydroxide, Mg(OH)2 (both 99% and 99.99% purity grades), γ-Al2O3, and AlOOH have been investigated for the direct production of transparent MgAl2O4. The highest average in-line transmittance through 3.5–4 mm thick samples is 84.2 ± 1.0% at 550 nm, attained by using mixtures of 99.99% pure Mg(OH)2 and γ-Al2O3. Other formulations exhibited 77–80% visible transmission, suggesting that further optimization can improve sample consistency. All samples exhibited a Knoop hardness of ~12 GPa, and elastic modulus of ~280 GPa. Biaxial flexural strength measurements ranged from 85 to 136 MPa depending on starting materials.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00673.x" xmlns="http://purl.org/rss/1.0/"><title>Dielectric and Mechanical Properties of Hot-Pressed Sintered Csf/Al2O3 Ceramic Composites</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00673.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Dielectric and Mechanical Properties of Hot-Pressed Sintered Csf/Al2O3 Ceramic Composites</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Zhibin Huang, Wancheng Zhou, Rufei Ma, Xiufeng Tang, Fa Luo, Jiankun Zhu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-21T12:11:07.730646-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00673.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00673.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00673.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>High densified C<sub>sf</sub>/Al<sub>2</sub>O<sub>3</sub> ceramic composites were prepared by hot-pressed sintering using α-Al<sub>2</sub>O<sub>3</sub> powders and short carbon fibers as starting materials. Dielectric and mechanical properties of these composites were evaluated. The results show that the addition of short carbon fiber (C<sub>sf</sub>) conducting fillers renders the composites radar absorbing ability, while the hardness around 90 HRF and strength around 300 MPa are also obtained in these composites. Both the fiber content and the length can be used to optimize the dielectric property at the frequency range 8.2–12.4 GHz. The results indicate that C<sub>sf</sub>/Al<sub>2</sub>O<sub>3</sub> composite is a promising radar absorbing material with load-bearing ability.</p></div>]]></content:encoded><description>High densified Csf/Al2O3 ceramic composites were prepared by hot-pressed sintering using α-Al2O3 powders and short carbon fibers as starting materials. Dielectric and mechanical properties of these composites were evaluated. The results show that the addition of short carbon fiber (Csf) conducting fillers renders the composites radar absorbing ability, while the hardness around 90 HRF and strength around 300 MPa are also obtained in these composites. Both the fiber content and the length can be used to optimize the dielectric property at the frequency range 8.2–12.4 GHz. The results indicate that Csf/Al2O3 composite is a promising radar absorbing material with load-bearing ability.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00677.x" xmlns="http://purl.org/rss/1.0/"><title>SiC Ceramic-Bonded Carbon Fabricated With Si3N4 and Carbon Powders</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00677.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">SiC Ceramic-Bonded Carbon Fabricated With Si3N4 and Carbon Powders</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Weiwu Chen, Tetsuro Tojo, Yoshinari Miyamoto</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-20T02:12:45.686503-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00677.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00677.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00677.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Topical Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>New composites called ceramic-bonded carbon (CBCs), consisting of a three-dimensional structure of carbon particles bonded with thin ceramic boundaries, were developed. To fabricate light and tough CBCs and to understand their reinforcing mechanism, Si<sub>3</sub>N<sub>4</sub> and carbon powders (25:75 in volume ratio) were gelcasted and then sintered by spark plasma sintering at temperatures of 1700–1900°C. The ceramic boundary of SiC was formed <em>in situ</em> at above 1700°C by the reaction of Si<sub>3</sub>N<sub>4</sub> and C. The sintered CBCs showed a unique microstructure consisting of carbon particles and ceramic boundaries of 15 μm in size and 0.5–3 μm in thickness, respectively. With an increase in sintering temperature, physical bonding of ceramic grains to the carbon particles was enhanced as the grain growth of SiC increased. The SiC/CBCs sintered at 1900°C were highly dense (97% theoretical density), lightweight (2.36 mg/m<sup>3</sup>), and had both relatively high bending strength and thermal conductivity (135 MPa and 140 W/mK, respectively).</p></div>]]></content:encoded><description>New composites called ceramic-bonded carbon (CBCs), consisting of a three-dimensional structure of carbon particles bonded with thin ceramic boundaries, were developed. To fabricate light and tough CBCs and to understand their reinforcing mechanism, Si3N4 and carbon powders (25:75 in volume ratio) were gelcasted and then sintered by spark plasma sintering at temperatures of 1700–1900°C. The ceramic boundary of SiC was formed in situ at above 1700°C by the reaction of Si3N4 and C. The sintered CBCs showed a unique microstructure consisting of carbon particles and ceramic boundaries of 15 μm in size and 0.5–3 μm in thickness, respectively. With an increase in sintering temperature, physical bonding of ceramic grains to the carbon particles was enhanced as the grain growth of SiC increased. The SiC/CBCs sintered at 1900°C were highly dense (97% theoretical density), lightweight (2.36 mg/m3), and had both relatively high bending strength and thermal conductivity (135 MPa and 140 W/mK, respectively).</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00670.x" xmlns="http://purl.org/rss/1.0/"><title>Quantification of Oxide Inclusions and Porosity Structure in a Tantalum Carbide Microstructure Fabricated From Carbothermal Reduced Tantalum Oxide Precursor Powders</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00670.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Quantification of Oxide Inclusions and Porosity Structure in a Tantalum Carbide Microstructure Fabricated From Carbothermal Reduced Tantalum Oxide Precursor Powders</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Robert A. Morris, Daniel Butts, Gregory B. Thompson</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-20T02:12:38.523608-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00670.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00670.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00670.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Topical Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The oxide inclusion and porosity defect structures in a tantalum carbide specimen fabricated from vacuum plasma spraying with postspraying sintering and hot-isostatic pressing has been characterized. The tantalum carbide powders were obtained using a carbothermal reduction process of tantalum oxide precursors. During its fabrication, oxide-based inclusions formed from intrinsic impurities in the powder. Using serial sectioning and three-dimensional reconstruction techniques, interconnected globular oxide inclusions were revealed to be within the matrix phase and in the grain boundaries. The oxide phase was identified to be <em>z</em>-Ta<sub>2</sub>O<sub>5</sub> through selected area electron diffraction. The two- and three-dimensional porosity size distribution was compared and accounted for ~2% of the volume.</p></div>]]></content:encoded><description>The oxide inclusion and porosity defect structures in a tantalum carbide specimen fabricated from vacuum plasma spraying with postspraying sintering and hot-isostatic pressing has been characterized. The tantalum carbide powders were obtained using a carbothermal reduction process of tantalum oxide precursors. During its fabrication, oxide-based inclusions formed from intrinsic impurities in the powder. Using serial sectioning and three-dimensional reconstruction techniques, interconnected globular oxide inclusions were revealed to be within the matrix phase and in the grain boundaries. The oxide phase was identified to be z-Ta2O5 through selected area electron diffraction. The two- and three-dimensional porosity size distribution was compared and accounted for ~2% of the volume.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00678.x" xmlns="http://purl.org/rss/1.0/"><title>Microwave Dielectric Properties of (1 − x)(Mg0.95Ni0.05)TiO3–x(Ca0.8Sr0.2)TiO3 Ceramic System With Near-Zero Temperature Coefficient</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00678.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Microwave Dielectric Properties of (1 − x)(Mg0.95Ni0.05)TiO3–x(Ca0.8Sr0.2)TiO3 Ceramic System With Near-Zero Temperature Coefficient</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Chun-Hsu Shen, Cheng-Liang Huang, Wei-Ting Chen, Chung-Long Pan</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-18T10:25:32.550324-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00678.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00678.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00678.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Topical Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The microwave dielectric properties of the (1 − <em>x</em>)(Mg<sub>0.95</sub>Ni<sub>0.05</sub>)TiO<sub>3</sub>–<em>x</em>(Ca<sub>0.8</sub>Sr<sub>0.2</sub>)TiO<sub>3</sub> ceramic system prepared by mixed oxide route have been investigated. The crystal structures and the microstructures of the ceramics were characterized by means X-ray and scanning electron microscopy. The microwave dielectric properties are strongly related to the density and matrix of the specimen. Combination of (Mg<sub>0.95</sub>Ni<sub>0.05</sub>)TiO<sub>3</sub> (ilmenite-type structure) and (Ca<sub>0.8</sub>Sr<sub>0.2</sub>)TiO<sub>3</sub> (perovskite-structured) forms a two-phase system and leads to a near-zero temperature coefficient (τ<sub>f</sub>). With increasing <em>x</em>, the quality factor (<em>Q </em>× <em>f</em>) decreased and dielectric constant (ε<sub>r</sub>) increased. A new microwave dielectric material 0.95(Mg<sub>0.95</sub>Ni<sub>0.05</sub>)TiO<sub>3</sub>–0.05(Ca<sub>0.8</sub>Sr<sub>0.2</sub>)TiO<sub>3</sub>, possessing excellent microwave dielectric properties with a dielectric constant (ε<sub>r</sub>) of 21.68, a quality factor (<em>Q </em>× <em>f</em>) of 94,000 (GHz) and a temperature coefficient (τ<sub>f</sub>) of approximately −5.2 ppm/°C at 1275°C for 4 h, is proposed as a suitable candidate material for microwave applications requiring low dielectric loss.</p></div>]]></content:encoded><description>The microwave dielectric properties of the (1 − x)(Mg0.95Ni0.05)TiO3–x(Ca0.8Sr0.2)TiO3 ceramic system prepared by mixed oxide route have been investigated. The crystal structures and the microstructures of the ceramics were characterized by means X-ray and scanning electron microscopy. The microwave dielectric properties are strongly related to the density and matrix of the specimen. Combination of (Mg0.95Ni0.05)TiO3 (ilmenite-type structure) and (Ca0.8Sr0.2)TiO3 (perovskite-structured) forms a two-phase system and leads to a near-zero temperature coefficient (τf). With increasing x, the quality factor (Q × f) decreased and dielectric constant (εr) increased. A new microwave dielectric material 0.95(Mg0.95Ni0.05)TiO3–0.05(Ca0.8Sr0.2)TiO3, possessing excellent microwave dielectric properties with a dielectric constant (εr) of 21.68, a quality factor (Q × f) of 94,000 (GHz) and a temperature coefficient (τf) of approximately −5.2 ppm/°C at 1275°C for 4 h, is proposed as a suitable candidate material for microwave applications requiring low dielectric loss.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00672.x" xmlns="http://purl.org/rss/1.0/"><title>Structural and Dielectric Studies of Nanocrystalline Calcium Substituted Magnesium Titanate Synthesized Through an Auto-Igniting Combustion Technique</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00672.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Structural and Dielectric Studies of Nanocrystalline Calcium Substituted Magnesium Titanate Synthesized Through an Auto-Igniting Combustion Technique</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Madukayil Kunjoonju Suresh, Jijimon Kumpukattu Thomas, Hariharan Sreemoolanadhan, Chandy Nellimmoottil George, Annamma John, Sam Solomon, Palakkattumala Ramachandra Sobhana Wariar, Jacob Koshy</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-18T10:25:01.086484-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00672.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00672.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00672.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Topical Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Nanocrystalline calcium substituted magnesium titanate was synthesized through an auto-igniting combustion technique. The phase constitution of the powder was examined using X-ray diffraction, thermal analyses, and spectroscopic studies. The particle size of ~30 nm was obtained, and that could be sintered to 96% of the theoretic density at 1150°C/2 h. The microstructure of the sintered surface was examined using scanning electron microscopy. The quality factor (<em>Q</em><sub>u</sub> ×<em> f </em>) of 65,110 GHz, dielectric constant (ε<sub>r</sub>) of 20.25, and temperature coefficient of resonant frequency (τ<sub>f</sub>) of ~0 ppm/°C suggest that the sintered sample can be used for microwave applications.</p></div>]]></content:encoded><description>Nanocrystalline calcium substituted magnesium titanate was synthesized through an auto-igniting combustion technique. The phase constitution of the powder was examined using X-ray diffraction, thermal analyses, and spectroscopic studies. The particle size of ~30 nm was obtained, and that could be sintered to 96% of the theoretic density at 1150°C/2 h. The microstructure of the sintered surface was examined using scanning electron microscopy. The quality factor (Qu × f ) of 65,110 GHz, dielectric constant (εr) of 20.25, and temperature coefficient of resonant frequency (τf) of ~0 ppm/°C suggest that the sintered sample can be used for microwave applications.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00669.x" xmlns="http://purl.org/rss/1.0/"><title>Preparation and Properties of Er-Doped ZrO2 Nanocrystalline Phase-Separated Preforms of Optical Fibers by MCVD Process</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00669.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Preparation and Properties of Er-Doped ZrO2 Nanocrystalline Phase-Separated Preforms of Optical Fibers by MCVD Process</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Anirban Dhar, Ivan Kasik, Bernard Dussardier, Ondrej Podrazky, Vlastimil Matejec</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-17T09:34:26.519369-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00669.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00669.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00669.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The fabrication of <span class="fixed-roman">Er</span>-doped <span class="fixed-roman">ZrO</span><sub>2</sub>-based nanocrystalline phase-separated silica optical preforms by the modified chemical vapor deposition process and solution-doping techniques is presented. Fabricated preform cores are nearly transparent and contain phase-separated rare-earth-doped nanocrystalline particles with diameters mainly in a range from 20 to 80 nm. High concentrations of erbium and aluminum in preform cores of about 0.3 and 14 mol%, respectively, have been achieved without defects on the core–cladding interface. Spectral losses in a range 800–1600 nm and fluorescence spectra of erbium ions around 1550 nm measured on a fiber drawn from the preform are reported.</p></div>]]></content:encoded><description>The fabrication of Er-doped ZrO2-based nanocrystalline phase-separated silica optical preforms by the modified chemical vapor deposition process and solution-doping techniques is presented. Fabricated preform cores are nearly transparent and contain phase-separated rare-earth-doped nanocrystalline particles with diameters mainly in a range from 20 to 80 nm. High concentrations of erbium and aluminum in preform cores of about 0.3 and 14 mol%, respectively, have been achieved without defects on the core–cladding interface. Spectral losses in a range 800–1600 nm and fluorescence spectra of erbium ions around 1550 nm measured on a fiber drawn from the preform are reported.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00674.x" xmlns="http://purl.org/rss/1.0/"><title>Deoxidization of V2O5 Powder into VO2 Assisted by an Electrochemical Lithium Intercalation Technique</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00674.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Deoxidization of V2O5 Powder into VO2 Assisted by an Electrochemical Lithium Intercalation Technique</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jikun Chen, Xinling Liu, Lidong Chen, Nuofu Chen, Lei Dai, Yanfeng Gao</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-07T15:33:11.375622-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2011.00674.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2011.00674.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2011.00674.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Topical Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>This article demonstrates a method to fabricate VO<sub>2</sub> powder by annealing a precursor that was obtained by electrochemical intercalation of lithium into layered structured <span class="fixed-roman">V</span><sub>2</sub><span class="fixed-roman">O</span><sub>5</sub>. The method includes three steps. First, <span class="fixed-roman">Li<sup>+</sup></span> was intercalated into interlayers of <span class="fixed-roman">V</span><sub>2</sub><span class="fixed-roman">O</span><sub>5</sub> through an electrochemical process with precisely controlled electrical discharging currents and intercalation amounts, and at the same time <span class="fixed-roman">V<sup>5+</sup></span> would be deoxidized into <span class="fixed-roman">V<sup>4+</sup></span>. Secondly, the <span class="fixed-roman">Li<sup>+</sup></span>-intercalated powder was rinsed in an acid solution to achieve an ion exchanging process of replacing the <span class="fixed-roman">Li<sup>+</sup></span> in the <span class="fixed-roman">V–O</span> frame with <span class="fixed-roman">H<sup>+</sup></span>. Thirdly, the powder was annealed at 800°C in <span class="fixed-roman">N<sub>2</sub></span> atmosphere for dehydration and <span class="fixed-roman">VO</span><sub>2</sub> crystallization. By DSC investigation, the as-produced final product has a strong endothermic peak at around 68°C in a heating semicycle, which is indicative of the phase transition from <span class="fixed-roman">VO</span><sub>2</sub>(M) to <span class="fixed-roman">VO</span><sub>2</sub>(R). This approach can be extended to the fabrication of other sub-valence oxides by lithium intercalation and deoxidization of its higher valence layer-structured precursors.</p></div>]]></content:encoded><description>This article demonstrates a method to fabricate VO2 powder by annealing a precursor that was obtained by electrochemical intercalation of lithium into layered structured V2O5. The method includes three steps. First, Li+ was intercalated into interlayers of V2O5 through an electrochemical process with precisely controlled electrical discharging currents and intercalation amounts, and at the same time V5+ would be deoxidized into V4+. Secondly, the Li+-intercalated powder was rinsed in an acid solution to achieve an ion exchanging process of replacing the Li+ in the V–O frame with H+. Thirdly, the powder was annealed at 800°C in N2 atmosphere for dehydration and VO2 crystallization. By DSC investigation, the as-produced final product has a strong endothermic peak at around 68°C in a heating semicycle, which is indicative of the phase transition from VO2(M) to VO2(R). This approach can be extended to the fabrication of other sub-valence oxides by lithium intercalation and deoxidization of its higher valence layer-structured precursors.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12089" xmlns="http://purl.org/rss/1.0/"><title>Emerging Opportunities in Ceramics: Reports from the 4th International Congress on Ceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12089</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Emerging Opportunities in Ceramics: Reports from the 4th International Congress on Ceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Katherine T. Faber, Edgar Lara-Curzio</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-25T14:00:57.678907-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12089</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12089</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12089</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Introductory Piece</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">377</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">378</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[]]></content:encoded><description/></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12038" xmlns="http://purl.org/rss/1.0/"><title>Workforce Development: Challenges and Opportunities for Ceramic Science and Engineering</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12038</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Workforce Development: Challenges and Opportunities for Ceramic Science and Engineering</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Lynnette D. Madsen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-11T10:41:05.331409-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12038</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12038</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12038</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">379</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">383</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>It remains both a challenge and an opportunity to attract and nurture the best talent in ceramic science and engineering. Success stories in other areas provide examples of how to do it. Research findings reveal behaviors and specific actions that encourage excellence in all individuals, for example, showing support, creating structures that promote interaction, and establishing clear expectations. In developing countries, where the education and research infrastructure are often not as strong and English is not otherwise the language of choice, additional factors come into play. Involving students in research and exchanges—both domestically and internationally—within academe and with other sectors are keys to maintaining a high level of engagement. Students need to identify with the benefits and goals of their career paths. It is imperative that the education curriculum be nimble and incorporate skill development in important and emerging areas such as entrepreneurship and integrated computation and modeling.</p></div>
]]></content:encoded><description>
It remains both a challenge and an opportunity to attract and nurture the best talent in ceramic science and engineering. Success stories in other areas provide examples of how to do it. Research findings reveal behaviors and specific actions that encourage excellence in all individuals, for example, showing support, creating structures that promote interaction, and establishing clear expectations. In developing countries, where the education and research infrastructure are often not as strong and English is not otherwise the language of choice, additional factors come into play. Involving students in research and exchanges—both domestically and internationally—within academe and with other sectors are keys to maintaining a high level of engagement. Students need to identify with the benefits and goals of their career paths. It is imperative that the education curriculum be nimble and incorporate skill development in important and emerging areas such as entrepreneurship and integrated computation and modeling.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12064" xmlns="http://purl.org/rss/1.0/"><title>Opportunities and Challenges in Biology and Medicine: A Report from the 4th International Congress on Ceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12064</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Opportunities and Challenges in Biology and Medicine: A Report from the 4th International Congress on Ceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Vivek Pawar</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-09T13:35:40.133288-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12064</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12064</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12064</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">384</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">388</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>This article summarizes the opportunities and challenges for future research in ceramics used in biology and medicine. The summary was prepared from the seven presentations at the 4th International Congress on Ceramics held from July 15 to 19, 2012, in Chicago, USA. The major emerging opportunities identified were as follows: (i) developing fundamental understanding of bioactive ions used in bioceramics, (ii) possibility of using novel manufacturing methods such as 3D printing, (iii) attaching bioceramics to metallic implants, and (iv) enabling collaboration between ceramicist, biologist, industry, and medical professionals.</p></div>
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This article summarizes the opportunities and challenges for future research in ceramics used in biology and medicine. The summary was prepared from the seven presentations at the 4th International Congress on Ceramics held from July 15 to 19, 2012, in Chicago, USA. The major emerging opportunities identified were as follows: (i) developing fundamental understanding of bioactive ions used in bioceramics, (ii) possibility of using novel manufacturing methods such as 3D printing, (iii) attaching bioceramics to metallic implants, and (iv) enabling collaboration between ceramicist, biologist, industry, and medical professionals.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12069" xmlns="http://purl.org/rss/1.0/"><title>Shaping the Future of Ceramics for Aerospace Applications</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12069</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Shaping the Future of Ceramics for Aerospace Applications</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Todd E. Steyer</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-09T13:35:56.713164-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12069</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12069</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12069</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">389</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">394</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Aerospace was one of several parallel tracks at the 4th International Congress on Ceramics. Three prominent areas for application of ceramic technology to aerospace were discussed: propulsion and exhaust washed structures, thermal protection systems, and hot primary structure. Whereas ceramics are not new to aerospace, their application heretofore has been rather limited. Beyond directly working the technical maturity of various ceramic matrix composite, thermal protection, and ultra-high-temperature ceramic materials and systems, specific efforts are required to fully transition these materials for aerospace applications, to nurture the technology through to application, and to address affordability.</p></div>
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Aerospace was one of several parallel tracks at the 4th International Congress on Ceramics. Three prominent areas for application of ceramic technology to aerospace were discussed: propulsion and exhaust washed structures, thermal protection systems, and hot primary structure. Whereas ceramics are not new to aerospace, their application heretofore has been rather limited. Beyond directly working the technical maturity of various ceramic matrix composite, thermal protection, and ultra-high-temperature ceramic materials and systems, specific efforts are required to fully transition these materials for aerospace applications, to nurture the technology through to application, and to address affordability.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12033" xmlns="http://purl.org/rss/1.0/"><title>Preliminary Model and Technology of Piezoelectric Low Temperature Co-fired Ceramic (LTCC) Uniaxial Accelerometer</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12033</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Preliminary Model and Technology of Piezoelectric Low Temperature Co-fired Ceramic (LTCC) Uniaxial Accelerometer</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dominik Jurków, Arkadiusz Dąbrowski, Leszek Golonka, Tomasz Zawada</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-25T14:00:57.678907-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12033</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12033</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12033</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">395</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">404</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Design procedure, technology and basic properties of a piezoelectric Low Temperature Co-fired Ceramics (LTCC) accelerometer are presented in this paper. The sensor consists of a LTCC membrane with a seismic mass. Meggitt InSensor<sup>®</sup> PZT thick film has been applied as the sensing material. Finite element method (FEM) has been used to analyze the impact of the sensor geometry (membrane thickness, membrane and seismic mass radii) and PZT thick film placement on basic properties (sensitivity and bandwidth) of the device. The LTCC process was optimized in order to create thin and planar ceramic membrane with relatively huge seismic mass. Selected properties of the sensor have been measured and compared with the simulated ones.</p></div>
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Design procedure, technology and basic properties of a piezoelectric Low Temperature Co-fired Ceramics (LTCC) accelerometer are presented in this paper. The sensor consists of a LTCC membrane with a seismic mass. Meggitt InSensor® PZT thick film has been applied as the sensing material. Finite element method (FEM) has been used to analyze the impact of the sensor geometry (membrane thickness, membrane and seismic mass radii) and PZT thick film placement on basic properties (sensitivity and bandwidth) of the device. The LTCC process was optimized in order to create thin and planar ceramic membrane with relatively huge seismic mass. Selected properties of the sensor have been measured and compared with the simulated ones.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12034" xmlns="http://purl.org/rss/1.0/"><title>Design and Fabrication of Transparent and Gas-Tight Optical Windows in Low-Temperature Co-Fired Ceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12034</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Design and Fabrication of Transparent and Gas-Tight Optical Windows in Low-Temperature Co-Fired Ceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Tilo Welker, Thomas Geiling, Heike Bartsch, Jens Müller</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-04T11:45:39.057598-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12034</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12034</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12034</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">405</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">412</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Low-temperature co-fired ceramics (LTCC) enable the fabrication of microfluidic elements such as channels and embedded cavities in electrical devices. Hence, LTCC facilitate the realization of complex and integrated microfluidic devices. Examples can be applied in many areas like reaction chambers for synthesis of chemical compounds. However, for many applications it is necessary to have an optically transparent interface to the surroundings. The integration of optical windows in LTCC opens up a wide field of new and innovative applications such as the observation of chemiluminescent reactions. These chemical reactions emit electromagnetic radiation and thus offer a method for noninvasive detection. Thin glasses (≤500 μm) were bonded by thermocompression onto a LTCC substrate. As the bonding agent, a glass frit paste was used. Borosilicate glasses, fused silica as well as silicon were successfully bonded onto LTCC. To join materials with a large coefficient of thermal expansion mismatch (i.e., fused silica and LTCC), it is necessary to limit the heat input to the bond interface. Therefore, a heating structure was integrated into the LTCC substrate beneath the bond interface. This bonding process provides a gas-tight optical port with a high bond strength.</p></div>
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Low-temperature co-fired ceramics (LTCC) enable the fabrication of microfluidic elements such as channels and embedded cavities in electrical devices. Hence, LTCC facilitate the realization of complex and integrated microfluidic devices. Examples can be applied in many areas like reaction chambers for synthesis of chemical compounds. However, for many applications it is necessary to have an optically transparent interface to the surroundings. The integration of optical windows in LTCC opens up a wide field of new and innovative applications such as the observation of chemiluminescent reactions. These chemical reactions emit electromagnetic radiation and thus offer a method for noninvasive detection. Thin glasses (≤500 μm) were bonded by thermocompression onto a LTCC substrate. As the bonding agent, a glass frit paste was used. Borosilicate glasses, fused silica as well as silicon were successfully bonded onto LTCC. To join materials with a large coefficient of thermal expansion mismatch (i.e., fused silica and LTCC), it is necessary to limit the heat input to the bond interface. Therefore, a heating structure was integrated into the LTCC substrate beneath the bond interface. This bonding process provides a gas-tight optical port with a high bond strength.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12052" xmlns="http://purl.org/rss/1.0/"><title>Low-Temperature Co-Fired Ceramic Substrates for High-Performance Strain Gauges</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12052</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Low-Temperature Co-Fired Ceramic Substrates for High-Performance Strain Gauges</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Bjoern Brandt, Marion Gemeinert, Torsten Rabe, Jochen Bolte</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-25T10:45:50.01293-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12052</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12052</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12052</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">413</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">420</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Recent advances in the development of high gauge factor thin films for strain gauges prompt the research on advanced substrate materials. A glass ceramic composite has been developed in consideration of a high coefficient of thermal expansion (9.4 ppm/K) and a low modulus of elasticity (82 GPa) for the application as support material for thin-film sensors. In the first part, constantan foil strain gauges were fabricated from this material by tape casting, pressure-assisted sintering, and subsequent lamination of the metal foil on the planar ceramic substrates. The accuracy of the assembled load cells corresponds to accuracy class C6. That qualifies the load cells for the use in automatic packaging units and confirms the applicability of the low-temperature co-fired ceramic (LTCC) substrates for fabrication of accurate strain gauges. In the second part, to facilitate the deposition of thin-film sensor structures to the LTCC substrates, pressure-assisted sintering step is modified using smooth setters instead of release tapes, which resulted in fabrication of substrates with low average surface roughness of 50 nm. Titanium thin films deposited on these substrates as test coatings exhibited low surface resistances of 850 Ω comparable to thin films on commercial alumina thin-film substrates with 920 Ω. The presented material design and advances in manufacturing technology are important to promote the development of high-performance thin-film strain gauges.</p></div>
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Recent advances in the development of high gauge factor thin films for strain gauges prompt the research on advanced substrate materials. A glass ceramic composite has been developed in consideration of a high coefficient of thermal expansion (9.4 ppm/K) and a low modulus of elasticity (82 GPa) for the application as support material for thin-film sensors. In the first part, constantan foil strain gauges were fabricated from this material by tape casting, pressure-assisted sintering, and subsequent lamination of the metal foil on the planar ceramic substrates. The accuracy of the assembled load cells corresponds to accuracy class C6. That qualifies the load cells for the use in automatic packaging units and confirms the applicability of the low-temperature co-fired ceramic (LTCC) substrates for fabrication of accurate strain gauges. In the second part, to facilitate the deposition of thin-film sensor structures to the LTCC substrates, pressure-assisted sintering step is modified using smooth setters instead of release tapes, which resulted in fabrication of substrates with low average surface roughness of 50 nm. Titanium thin films deposited on these substrates as test coatings exhibited low surface resistances of 850 Ω comparable to thin films on commercial alumina thin-film substrates with 920 Ω. The presented material design and advances in manufacturing technology are important to promote the development of high-performance thin-film strain gauges.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12040" xmlns="http://purl.org/rss/1.0/"><title>Application of Thin-Film Manufacturing Technologies to Solid Oxide Fuel Cells and Gas Separation Membranes</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12040</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Application of Thin-Film Manufacturing Technologies to Solid Oxide Fuel Cells and Gas Separation Membranes</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Norbert H. Menzler, Feng Han, Tim Gestel, Wolfgang Schafbauer, Falk Schulze-Küppers, Stefan Baumann, Sven Uhlenbruck, Wilhelm A. Meulenberg, Ludger Blum, Hans Peter Buchkremer</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-21T13:10:38.002902-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12040</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12040</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12040</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">421</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">427</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The implementation of thin-film technologies in energy-related applications, such as special fuel cells and gas separation membranes for low-emission power plants, is essential in terms of enhancing the functionality, reducing operating temperatures, and increasing lifetime. Introducing thin electrolyte layers into solid oxide fuel cells (SOFCs) decreases the internal cell resistance and thus drastically enhances the power density. This supports the goal of reducing the operation temperature from ~800°C to temperatures below 700°C. As the operation temperature is lowered, the temperature-activated degradation processes are slowed down, and 40,000 h of operation becomes feasible. Reducing the thickness of the gas separation membranes also reduces internal losses, and therefore, the rate-limiting steps within the layer. Thinner functional layers possess higher permeabilities but also involve a risk of more layer defects. This also holds for the fuel cells. Thus, the manufacturing of the supports and the intermediate layers is also very important. The paper gives an overview of the application of thin-film technologies to SOFCs and gas separation membranes and highlights the efforts to date. Examples include SOFC stacks operated stably for in excess of 40,000 h and submicron-sized membranes with high permeability and good separation factors.</p></div>
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The implementation of thin-film technologies in energy-related applications, such as special fuel cells and gas separation membranes for low-emission power plants, is essential in terms of enhancing the functionality, reducing operating temperatures, and increasing lifetime. Introducing thin electrolyte layers into solid oxide fuel cells (SOFCs) decreases the internal cell resistance and thus drastically enhances the power density. This supports the goal of reducing the operation temperature from ~800°C to temperatures below 700°C. As the operation temperature is lowered, the temperature-activated degradation processes are slowed down, and 40,000 h of operation becomes feasible. Reducing the thickness of the gas separation membranes also reduces internal losses, and therefore, the rate-limiting steps within the layer. Thinner functional layers possess higher permeabilities but also involve a risk of more layer defects. This also holds for the fuel cells. Thus, the manufacturing of the supports and the intermediate layers is also very important. The paper gives an overview of the application of thin-film technologies to SOFCs and gas separation membranes and highlights the efforts to date. Examples include SOFC stacks operated stably for in excess of 40,000 h and submicron-sized membranes with high permeability and good separation factors.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12045" xmlns="http://purl.org/rss/1.0/"><title>Low-Temperature Sintered NTC Thermistor Ceramics for Thick-Film Temperature Sensors</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12045</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Low-Temperature Sintered NTC Thermistor Ceramics for Thick-Film Temperature Sensors</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Timmy Reimann, Jörg Töpfer, Stefan Barth, Heike Bartsch, Jens Müller</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-21T13:10:47.616875-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12045</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12045</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12045</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">428</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">434</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Negative temperature coefficient (NTC) thermistor thick films were fabricated by screen printing on alumina substrates and firing at 900°C. Spinel-type <span class="fixed-roman">NiMn</span><sub>2</sub><span class="fixed-roman">O</span><sub>4</sub> exhibits limited stability in air between 730 and 970°C only and interacts with the <span class="fixed-roman">Bi<sub>2</sub>O<sub>3</sub></span> additive. The <span class="fixed-roman">Zn–Co</span>-substituted spinel <span class="fixed-roman">Zn</span><sub>0.75</sub><span class="fixed-roman">Ni</span><sub>0.5</sub><span class="fixed-roman">Co</span><sub>0.5</sub><span class="fixed-roman">Mn</span><sub>1.25</sub><span class="fixed-roman">O</span><sub>4</sub> with 3 wt% additive shows complete densification at 900°C; no interaction between spinel and additive was observed. Alternatively, a <span class="fixed-roman">Cu–Zn–Co</span>-substituted <span class="fixed-roman">Cu</span><sub>0.37</sub><span class="fixed-roman">Zn</span><sub>0.52</sub><span class="fixed-roman">Ni</span><sub>0.44</sub><span class="fixed-roman">Co</span><sub>0.44</sub><span class="fixed-roman">Mn</span><sub>1.23</sub><span class="fixed-roman">O</span><sub>4</sub> spinel with excellent sintering characteristics even without sintering additive was investigated. The thermistor films display a sheet resistance of about 300 kΩ/□ and B = 3300 K. The firing behavior, microstructure formation, and electrical properties of NTC thick films are reported.</p></div>
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Negative temperature coefficient (NTC) thermistor thick films were fabricated by screen printing on alumina substrates and firing at 900°C. Spinel-type NiMn2O4 exhibits limited stability in air between 730 and 970°C only and interacts with the Bi2O3 additive. The Zn–Co-substituted spinel Zn0.75Ni0.5Co0.5Mn1.25O4 with 3 wt% additive shows complete densification at 900°C; no interaction between spinel and additive was observed. Alternatively, a Cu–Zn–Co-substituted Cu0.37Zn0.52Ni0.44Co0.44Mn1.23O4 spinel with excellent sintering characteristics even without sintering additive was investigated. The thermistor films display a sheet resistance of about 300 kΩ/□ and B = 3300 K. The firing behavior, microstructure formation, and electrical properties of NTC thick films are reported.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12037" xmlns="http://purl.org/rss/1.0/"><title>Manufacturing and Characterization of a Deformable Membrane with Integrated Temperature Sensors and Heating Structures in Low Temperature Co-fired Ceramics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12037</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Manufacturing and Characterization of a Deformable Membrane with Integrated Temperature Sensors and Heating Structures in Low Temperature Co-fired Ceramics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Nam Gutzeit, Jens Müller, Claudia Reinlein, Sylvia Gebhardt</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-10T11:05:41.25119-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12037</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12037</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12037</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">435</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">442</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>In this article, the challenging manufacturing process of a deformable mirror for the wave front correction of a high energy laser is described. During this process, the low temperature co-fired ceramic (LTCC) membrane as the base component with integrated sensors must endure several postfire processes at temperatures of up to 900°C without any degradation of the sensors' characteristics. To optimize the sensors, various combinations of resistor and conductor pastes and different geometries are characterized. The usability and the performance of the sensor elements after temperature treatment are investigated by measuring the resistance and its resistance temperature characteristic.</p></div>
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In this article, the challenging manufacturing process of a deformable mirror for the wave front correction of a high energy laser is described. During this process, the low temperature co-fired ceramic (LTCC) membrane as the base component with integrated sensors must endure several postfire processes at temperatures of up to 900°C without any degradation of the sensors' characteristics. To optimize the sensors, various combinations of resistor and conductor pastes and different geometries are characterized. The usability and the performance of the sensor elements after temperature treatment are investigated by measuring the resistance and its resistance temperature characteristic.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12036" xmlns="http://purl.org/rss/1.0/"><title>Low-Temperature Co-Fired Ceramics System for Light Absorbance Measurement</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12036</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Low-Temperature Co-Fired Ceramics System for Light Absorbance Measurement</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mateusz J. Czok, Paweł I. Bembnowicz, Leszek J. Golonka</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-10T11:05:38.424653-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12036</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12036</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12036</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">443</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">448</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The article describes technology of the low-temperature co-fired ceramics (LTCC) structure that enables light absorbance measurements of liquid sample. The manufactured ceramic structure contains buried microfluidic channels. The structure consists of two co-fired glass windows that separate the light source and detector from the test solution. A construction of an electronic measurement system is described as well. The signal from three light-emitting diodes (LED)s — red, green, and blue — can be used in the absorbance measurements. The light intensity is measured by the TCS 3414CS (TAOS, Plano, TX) color detector. Optical properties of the fabricated microfluidic LTCC system is investigated with several concentrations of potassium permanganate (KMnO<sub>4</sub>) in water solution. The system can be applied in microbiology for constant monitoring of bacterial growth.</p></div>
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The article describes technology of the low-temperature co-fired ceramics (LTCC) structure that enables light absorbance measurements of liquid sample. The manufactured ceramic structure contains buried microfluidic channels. The structure consists of two co-fired glass windows that separate the light source and detector from the test solution. A construction of an electronic measurement system is described as well. The signal from three light-emitting diodes (LED)s — red, green, and blue — can be used in the absorbance measurements. The light intensity is measured by the TCS 3414CS (TAOS, Plano, TX) color detector. Optical properties of the fabricated microfluidic LTCC system is investigated with several concentrations of potassium permanganate (KMnO4) in water solution. The system can be applied in microbiology for constant monitoring of bacterial growth.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12030" xmlns="http://purl.org/rss/1.0/"><title>The Effect of Phase Composition on the Mechanical Properties of LTCC Material</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12030</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">The Effect of Phase Composition on the Mechanical Properties of LTCC Material</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Kostja Makarovič, Raul Bermejo, Irina Kraleva, Andreja Benčan, Marko Hrovat, Janez Holc, Barbara Malič, Marija Kosec</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-04T11:45:10.45555-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12030</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12030</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12030</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">449</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">457</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>For the fabrication of complex, micro-electromechanical systems (MEMS) devices based on low-temperature co-fired ceramic (LTCC), higher firing temperatures and longer times than those proposed by the LTCC producer are needed. These changes to the thermal budget may influence the material properties and consequently its functional properties. The effect of the firing conditions on the LTCC DuPont 951 and thus on the phase composition, that is, the alumina/anorthite ratio and porosity, on the mechanical properties is presented. The samples fired at low temperatures (800°C) had a high porosity (7%), which significantly contributed to the low elastic modulus (100 GPa) and the low mechanical strength of the LTCC (140 MPa). The samples fired at 850°C, which had only 1% of porosity, resulted in an elastic modulus of 122 GPa and a flexural strength of 224 MPa. A further increase in the temperature contributed to a slight decrease in the elastic modulus, while no significant difference in the flexural strength could be observed. The enhancement of the flexural strength with an increasing firing temperature was mainly related to a decrease in the porosity and to a lesser extent to the different ratio of the alumina/anorthite phases. The effect of firing time on the phase composition at selected temperatures (i.e., 100 h at 700 and 800°C) is also discussed.</p></div>
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For the fabrication of complex, micro-electromechanical systems (MEMS) devices based on low-temperature co-fired ceramic (LTCC), higher firing temperatures and longer times than those proposed by the LTCC producer are needed. These changes to the thermal budget may influence the material properties and consequently its functional properties. The effect of the firing conditions on the LTCC DuPont 951 and thus on the phase composition, that is, the alumina/anorthite ratio and porosity, on the mechanical properties is presented. The samples fired at low temperatures (800°C) had a high porosity (7%), which significantly contributed to the low elastic modulus (100 GPa) and the low mechanical strength of the LTCC (140 MPa). The samples fired at 850°C, which had only 1% of porosity, resulted in an elastic modulus of 122 GPa and a flexural strength of 224 MPa. A further increase in the temperature contributed to a slight decrease in the elastic modulus, while no significant difference in the flexural strength could be observed. The enhancement of the flexural strength with an increasing firing temperature was mainly related to a decrease in the porosity and to a lesser extent to the different ratio of the alumina/anorthite phases. The effect of firing time on the phase composition at selected temperatures (i.e., 100 h at 700 and 800°C) is also discussed.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12051" xmlns="http://purl.org/rss/1.0/"><title>Characterization of the Fabrication Process of Rolled LTCC Structures</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12051</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Characterization of the Fabrication Process of Rolled LTCC Structures</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Kelci Parrish, Mallory Yates, Derek Reis, Donald Plumlee, Jesse Taff</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-09T13:35:44.005046-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12051</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12051</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12051</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">458</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">467</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>This work focuses on the fabrication and assembly of cylindrical plasma containment tubes using DuPont's 951 low temperature co-fired ceramics (LTCC) for use in miniature electrostatic thrusters. The tube is used to contain argon plasma, which is generated by a spiral inductively coupled plasma antenna, which is also fabricated in LTCC. The tube also interfaces with two electrically biased grids on the opposite end, which accelerate the plasma out of the tube. These interfaces are highly dependent on the dimensions and tolerances of the containment tube. The development of the fabrication process will be presented for the incorporation of the tubes and grids onto the base as a single structure. This includes constructing the antenna base, shaping the “rolled” LTCC containment tube using a jig and isostatic press, and integrating the tube and antenna base during the firing. Following the fabrication, measurements will be taken to determine tube circularity and hermeticity of the seal at the interface between the tube and the antenna base. The results will be presented and characterized to evaluate the effectiveness of the structure as well as the documentation of the development of a rolled LTCC tube structure integrated with a planar LTCC antenna base.</p></div>
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This work focuses on the fabrication and assembly of cylindrical plasma containment tubes using DuPont's 951 low temperature co-fired ceramics (LTCC) for use in miniature electrostatic thrusters. The tube is used to contain argon plasma, which is generated by a spiral inductively coupled plasma antenna, which is also fabricated in LTCC. The tube also interfaces with two electrically biased grids on the opposite end, which accelerate the plasma out of the tube. These interfaces are highly dependent on the dimensions and tolerances of the containment tube. The development of the fabrication process will be presented for the incorporation of the tubes and grids onto the base as a single structure. This includes constructing the antenna base, shaping the “rolled” LTCC containment tube using a jig and isostatic press, and integrating the tube and antenna base during the firing. Following the fabrication, measurements will be taken to determine tube circularity and hermeticity of the seal at the interface between the tube and the antenna base. The results will be presented and characterized to evaluate the effectiveness of the structure as well as the documentation of the development of a rolled LTCC tube structure integrated with a planar LTCC antenna base.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12039" xmlns="http://purl.org/rss/1.0/"><title>Creation of Titania Artificial Interfaces with Geometric Patterns by Using Microstereolithography and Aqueous Solution Techniques</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12039</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Creation of Titania Artificial Interfaces with Geometric Patterns by Using Microstereolithography and Aqueous Solution Techniques</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Soshu Kirihara, Yusuke Itakura, Satoko Tasaki</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-09T13:35:24.844844-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/ijac.12039</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/ijac.12039</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fijac.12039</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">468</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">473</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Titania micropatterns with periodic arrangements were successfully formed on glass substrates for use with electromagnetic wave energy resonance and localizations in terahertz frequency ranges. Geometric arrangements of acrylic polygonal tablets with titania particle dispersions were fabricated by using micropatterning stereolithography. Moreover, periodically arranged full anatase-phase titania tablets were created homogeneously through liquid-phase crystal depositions of water solvent processes, using microtemplates fabricated by using the stereolithography system. The terahertz wave properties were measured and calculated by using a time-domain spectroscopic system and finite-difference time-domain method.</p></div>
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Titania micropatterns with periodic arrangements were successfully formed on glass substrates for use with electromagnetic wave energy resonance and localizations in terahertz frequency ranges. Geometric arrangements of acrylic polygonal tablets with titania particle dispersions were fabricated by using micropatterning stereolithography. Moreover, periodically arranged full anatase-phase titania tablets were created homogeneously through liquid-phase crystal depositions of water solvent processes, using microtemplates fabricated by using the stereolithography system. The terahertz wave properties were measured and calculated by using a time-domain spectroscopic system and finite-difference time-domain method.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02751.x" xmlns="http://purl.org/rss/1.0/"><title>Evaluation of Compacted Cementitious Composites for Porous Bearings</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02751.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Evaluation of Compacted Cementitious Composites for Porous Bearings</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Tulio H. Panzera, Andre L. Christoforo, Juan C. Campos Rubio, Christopher R. Bowen, Paulo H. Ribeiro Borges, Leandro J. Silva</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-02-15T15:04:48.073316-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02751.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02751.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02751.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">474</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">483</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The use of porous materials as a restrictor in aerostatic bearings provides many advantages over conventional restrictors, such as small variation of temperature, high damping, high operational speeds, limited wear, and capacity to support radial, axial, and combined loading. A design of experiment (DOE) was carried out to evaluate cold-pressed cementitious composites as an air restrictor in thrust bearings. The physical and mechanical properties such as the apparent porosity, permeability, and elastic modulus were investigated in this work, thus verifying the structural and flow characteristics of the composites for such application. The composites fabricated with low compacting pressure and small silica particles provided the material requirements for porous bearings.</p></div>
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The use of porous materials as a restrictor in aerostatic bearings provides many advantages over conventional restrictors, such as small variation of temperature, high damping, high operational speeds, limited wear, and capacity to support radial, axial, and combined loading. A design of experiment (DOE) was carried out to evaluate cold-pressed cementitious composites as an air restrictor in thrust bearings. The physical and mechanical properties such as the apparent porosity, permeability, and elastic modulus were investigated in this work, thus verifying the structural and flow characteristics of the composites for such application. The composites fabricated with low compacting pressure and small silica particles provided the material requirements for porous bearings.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02752.x" xmlns="http://purl.org/rss/1.0/"><title>Laser Machining and Functional Applications of Glass-Ceramic Materials</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02752.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Laser Machining and Functional Applications of Glass-Ceramic Materials</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Daniel Sola, Jose I. Peña</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-02-16T13:58:29.56719-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02752.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02752.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02752.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">484</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">491</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>In this work a study of glass-ceramic laser machining and some functional applications are presented. Firstly, both the effect produced by the machining method as well as how the modification of the reference position influence the machining results have been studied. Secondly, blind holes and special shape cross-section blind holes have been created for functional purposes. A Q-switched Nd:YAG laser at its fundamental wavelength of 1064 nm with pulse-widths in the nanosecond range has been used. Morphology, depth, and volume obtained by machining grooves have been studied. The variation in the ablation yield when the position of the surface to be machined is modified has also been studied. The composition and microstructure of the machined areas have been described and discussed and thermal tests have been performed to check if the objectives of the functional applications have been achieved.</p></div>
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In this work a study of glass-ceramic laser machining and some functional applications are presented. Firstly, both the effect produced by the machining method as well as how the modification of the reference position influence the machining results have been studied. Secondly, blind holes and special shape cross-section blind holes have been created for functional purposes. A Q-switched Nd:YAG laser at its fundamental wavelength of 1064 nm with pulse-widths in the nanosecond range has been used. Morphology, depth, and volume obtained by machining grooves have been studied. The variation in the ablation yield when the position of the surface to be machined is modified has also been studied. The composition and microstructure of the machined areas have been described and discussed and thermal tests have been performed to check if the objectives of the functional applications have been achieved.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02754.x" xmlns="http://purl.org/rss/1.0/"><title>Silver Co-Firable Li2ZnTi3O8 Microwave Dielectric Ceramics with LZB Glass Additive and TiO2 Dopant</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02754.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Silver Co-Firable Li2ZnTi3O8 Microwave Dielectric Ceramics with LZB Glass Additive and TiO2 Dopant</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Guohua Chen, Meizhen Hou, Yan Bao, Changlai Yuan, Changrong Zhou, Huarui Xu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-02-13T12:37:28.888727-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02754.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02754.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02754.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">492</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">501</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>New dielectric ceramics are prepared by the conventional solid-state ceramic route. Effects of LZB glass on sintering, phase purity, microstructure, and dielectric properties of <span class="fixed-roman">Li<sub>2</sub>ZnTi<sub>3</sub>O<sub>8</sub></span> ceramics have been investigated. Adding LZB lowers sintering temperature from 1050°C to 875°C, and does not induce much degradation of dielectric properties. The 1.0 wt% LZB glass-added ceramic has better properties of ε<sub><em>r</em></sub> = 23.9, <em>Q</em> × <em>f </em>=<em> </em>31,608 GHz, τ<sub><em>f</em></sub> = −14.3 ppm/°C. Additions of <span class="fixed-roman">TiO<sub>2</sub></span> markedly improve microwave properties. Typically, the <span class="fixed-roman">Li<sub>2</sub>ZnTi<sub>3</sub>O<sub>8</sub></span> + 1 wt%LZB + 3.5 wt%<span class="fixed-roman">TiO<sub>2</sub></span> sintered at 900°C shows ε<sub><em>r</em></sub> = 26.1, <em>Q</em> × <em>f </em>=<em> </em>45,168 GHz, τ<sub><em>f</em></sub><em> </em>= −4.1 ppm/°C. Compatibility with Ag electrode indicates that this material may be applied to LTCC devices.</p></div>
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New dielectric ceramics are prepared by the conventional solid-state ceramic route. Effects of LZB glass on sintering, phase purity, microstructure, and dielectric properties of Li2ZnTi3O8 ceramics have been investigated. Adding LZB lowers sintering temperature from 1050°C to 875°C, and does not induce much degradation of dielectric properties. The 1.0 wt% LZB glass-added ceramic has better properties of εr = 23.9, Q × f = 31,608 GHz, τf = −14.3 ppm/°C. Additions of TiO2 markedly improve microwave properties. Typically, the Li2ZnTi3O8 + 1 wt%LZB + 3.5 wt%TiO2 sintered at 900°C shows εr = 26.1, Q × f = 45,168 GHz, τf = −4.1 ppm/°C. Compatibility with Ag electrode indicates that this material may be applied to LTCC devices.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02755.x" xmlns="http://purl.org/rss/1.0/"><title>Effect of Polyacrylic Acid Addition on Rheology of SiC-Al2O3-ZrO2(3Y) Mixed Suspensions</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02755.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of Polyacrylic Acid Addition on Rheology of SiC-Al2O3-ZrO2(3Y) Mixed Suspensions</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ning Zhang, Bin Liang, Xiaojun Zhao, Xingyu Cui, Hongmin Kan, Hao Liu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-03-13T16:23:11.728958-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02755.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02755.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02755.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">502</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">508</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A suspension with good rheology and high stability is crucial for slip casting and gelcasting technology. However, a mixed suspension from two or more different powders usually has bad rheology because of the easy agglomeration of mixed powders caused by the attractive force between the powders with heterocharges. We studied the surface modification of the each single-component powders (<span class="fixed-roman">SiC</span>, <span class="fixed-roman">Al<sub>2</sub>O<sub>3</sub></span>, <span class="fixed-roman">ZrO<sub>2</sub></span>(3Y) powders) and the <span class="fixed-roman">SiC</span>-<span class="fixed-roman">Al<sub>2</sub>O<sub>3</sub></span>-<span class="fixed-roman">ZrO<sub>2</sub></span>(3Y) mixed powders to increase the repulsive force by adjusting the pH value and adding polyacrylic acid (PAA) as dispersant. The PAA addition effects on the <span class="fixed-roman">SiC</span>-<span class="fixed-roman">Al<sub>2</sub>O<sub>3</sub></span>-<span class="fixed-roman">ZrO<sub>2</sub></span>(3Y) mixture were investigated in terms of zeta potential, pH range for heterocharge region, dispersion of the mixed powders and rheology of the mixed slurry based on the study of each unary suspensions. The results show that before surface modification the <span class="fixed-roman">SiC</span>-<span class="fixed-roman">Al<sub>2</sub>O<sub>3</sub></span>-<span class="fixed-roman">ZrO<sub>2</sub></span>(3Y) mixed powders were agglomerated severely because they were in the heterocharge region with a broad pH range from 3.5 to 8.25, while after surface modification (pH = 10.5, PAA = 0.8wt%) the heterocharge region was narrowed with a relatively narrower pH range from 2.6 to 3.7. The mixed powders with homocharges were dispersed well because of the great electrostatic repulsive force and steric hindrance offered by PAA and the mixed suspensions had favorable rheology.</p></div>
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A suspension with good rheology and high stability is crucial for slip casting and gelcasting technology. However, a mixed suspension from two or more different powders usually has bad rheology because of the easy agglomeration of mixed powders caused by the attractive force between the powders with heterocharges. We studied the surface modification of the each single-component powders (SiC, Al2O3, ZrO2(3Y) powders) and the SiC-Al2O3-ZrO2(3Y) mixed powders to increase the repulsive force by adjusting the pH value and adding polyacrylic acid (PAA) as dispersant. The PAA addition effects on the SiC-Al2O3-ZrO2(3Y) mixture were investigated in terms of zeta potential, pH range for heterocharge region, dispersion of the mixed powders and rheology of the mixed slurry based on the study of each unary suspensions. The results show that before surface modification the SiC-Al2O3-ZrO2(3Y) mixed powders were agglomerated severely because they were in the heterocharge region with a broad pH range from 3.5 to 8.25, while after surface modification (pH = 10.5, PAA = 0.8wt%) the heterocharge region was narrowed with a relatively narrower pH range from 2.6 to 3.7. The mixed powders with homocharges were dispersed well because of the great electrostatic repulsive force and steric hindrance offered by PAA and the mixed suspensions had favorable rheology.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02756.x" xmlns="http://purl.org/rss/1.0/"><title>Development of Electrical Discharge Machinable ZTA Ceramics with 24 vol% of TiC, TiN, TiCN, TiB2 and WC as Electrically Conductive Phase</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02756.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Development of Electrical Discharge Machinable ZTA Ceramics with 24 vol% of TiC, TiN, TiCN, TiB2 and WC as Electrically Conductive Phase</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Richard Landfried, Frank Kern, Wolfgang Burger, Wolfgang Leonhardt, Rainer Gadow</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-03-13T16:23:51.043006-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02756.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02756.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02756.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">509</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">518</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>In order to develop ED-machinable ceramics with high strength, toughness and wear resistance, ZTA was chosen as matrix material. A dispersion of 24 vol% electrically conductive phase (<span class="fixed-roman">TiC</span>, <span class="fixed-roman">TiN</span>, <span class="fixed-roman">TiCN</span>, <span class="fixed-roman">TiB<sub>2</sub></span> and <span class="fixed-roman">WC</span>) was added. These composites were hot pressed for 1 h at 60 MPa and temperatures ranging from 1475°C to 1550°C. Mechanical and electrical properties were investigated. The influence of the electrically conductive phase on the surface quality after EDM was analyzed. The mechanical properties and machining quality were found to depend significantly on the type of conductive phase added. Machining of a complex shaped ZTA-<span class="fixed-roman">TiC</span> component was demonstrated.</p></div>
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In order to develop ED-machinable ceramics with high strength, toughness and wear resistance, ZTA was chosen as matrix material. A dispersion of 24 vol% electrically conductive phase (TiC, TiN, TiCN, TiB2 and WC) was added. These composites were hot pressed for 1 h at 60 MPa and temperatures ranging from 1475°C to 1550°C. Mechanical and electrical properties were investigated. The influence of the electrically conductive phase on the surface quality after EDM was analyzed. The mechanical properties and machining quality were found to depend significantly on the type of conductive phase added. Machining of a complex shaped ZTA-TiC component was demonstrated.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02758.x" xmlns="http://purl.org/rss/1.0/"><title>Influence of Phenolic Resin Impregnation on the Properties of Reaction-Bonded Silicon Carbide</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02758.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Influence of Phenolic Resin Impregnation on the Properties of Reaction-Bonded Silicon Carbide</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Zhaohua Luo, Dongliang Jiang, Jingxian Zhang, Qingling Lin, Zhongming Chen, Zhengren Huang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-03-13T16:25:32.224587-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02758.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02758.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02758.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">519</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">526</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Reaction-bonded silicon carbide ceramics fabricated from tape casting and Si infiltration have been reported in previous studies. To reduce the residual Si content in the sintered bodies, impregnation of phenol–formaldehyde resin (PF) into the porous green preforms before Si infiltration was proposed and studied in this work. The impregnation of PF solution not only helped to reduce the porosity and increase the carbon content of the green preforms, but also improved their strength. As a result, the flexural strength of the RBSC increased a lot and reached 856 ± 161MPa, whereas the residual Si content was reduced to 10 vol%.</p></div>
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Reaction-bonded silicon carbide ceramics fabricated from tape casting and Si infiltration have been reported in previous studies. To reduce the residual Si content in the sintered bodies, impregnation of phenol–formaldehyde resin (PF) into the porous green preforms before Si infiltration was proposed and studied in this work. The impregnation of PF solution not only helped to reduce the porosity and increase the carbon content of the green preforms, but also improved their strength. As a result, the flexural strength of the RBSC increased a lot and reached 856 ± 161MPa, whereas the residual Si content was reduced to 10 vol%.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02760.x" xmlns="http://purl.org/rss/1.0/"><title>Phase Evolution of Ti3SiC2 Annealing in Vacuum at Elevated Temperatures</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02760.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Phase Evolution of Ti3SiC2 Annealing in Vacuum at Elevated Temperatures</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Junling Zeng, Shufang Ren, Jinjun Lu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-03-08T04:14:22.903599-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02760.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02760.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02760.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">527</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">539</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The thermal decomposition of <span class="fixed-roman">T</span>i<sub>3</sub><span class="fixed-roman">S</span>i<span class="fixed-roman">C</span><sub>2</sub> in vacuum furnace up to 1500°C has been investigated. The results show that the mild decomposition of <span class="fixed-roman">T</span>i<sub>3</sub><span class="fixed-roman">S</span>i<span class="fixed-roman">C</span><sub>2</sub> commences at 1300°C and the higher the holding temperature, the larger the volatilization of Si atoms. The <span class="fixed-roman">T</span>i<sub>3</sub><span class="fixed-roman">S</span>i<span class="fixed-roman">C</span><sub>2</sub> decomposition occurs simultaneously on the surface and in the bulk. Four phases coexist at 1400°C and 1450°C and the Ti<sub>5</sub>Si<sub>3</sub>C<sub>x</sub> phase appears in the bulk and/or surface. Diffusion distance, rate, and volatilization of Si contribute to the porous structure and the presence of Ti<sub>5</sub>Si<sub>3</sub>C<sub>x</sub>. The evolution of furnace pressure reflects the decomposition kinetics of <span class="fixed-roman">T</span>i<sub>3</sub><span class="fixed-roman">S</span>i<span class="fixed-roman">C</span><sub>2</sub>.</p></div>
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The thermal decomposition of Ti3SiC2 in vacuum furnace up to 1500°C has been investigated. The results show that the mild decomposition of Ti3SiC2 commences at 1300°C and the higher the holding temperature, the larger the volatilization of Si atoms. The Ti3SiC2 decomposition occurs simultaneously on the surface and in the bulk. Four phases coexist at 1400°C and 1450°C and the Ti5Si3Cx phase appears in the bulk and/or surface. Diffusion distance, rate, and volatilization of Si contribute to the porous structure and the presence of Ti5Si3Cx. The evolution of furnace pressure reflects the decomposition kinetics of Ti3SiC2.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02761.x" xmlns="http://purl.org/rss/1.0/"><title>Variations in Tantalum Carbide Microstructures with Changing Carbon Content</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02761.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Variations in Tantalum Carbide Microstructures with Changing Carbon Content</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Robert A. Morris, Billie Wang, Daniel Butts, Gregory B. Thompson</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-03-08T12:27:05.163715-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02761.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02761.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02761.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">540</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">551</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A wide variety of microstructures have been obtained by vacuum plasma spraying (VPS) 39Ta:61C atomic percent feedstock powders. During processing, the powder feed was fed through a high energy VPS plasma plume, where altering nozzle angle changed the overall retained carbon concentration in the deposited material. The samples were subsequently sintered and hot isostatic pressed to homogenize and consolidate the microstructure. The microstructures consisted of grains that were either equiaxed or acicular. In the samples with less carbon loss, the equiaxed grains were either the TaC phase or a TaC matrix that encased fine laths of Ta<sub>4</sub>C<sub>3</sub>. In the sample with the most carbon loss, acicular grains were found containing layered and parallel TaC, Ta<sub>2</sub>C, and Ta<sub>4</sub>C<sub>3</sub> laths along the major-axis of the grains. The phases of the compounds have been determined by using complimentary X-ray diffraction and electron diffraction techniques. Focused ion beam serial sectioning and transmission electron microscopy tilt series tomography were performed to generate three-dimensional reconstructions of the microstructure morphologies. This article addresses how tantalum carbide microstructures are controlled by the overall concentration and phase fraction content in each of these samples.</p></div>
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A wide variety of microstructures have been obtained by vacuum plasma spraying (VPS) 39Ta:61C atomic percent feedstock powders. During processing, the powder feed was fed through a high energy VPS plasma plume, where altering nozzle angle changed the overall retained carbon concentration in the deposited material. The samples were subsequently sintered and hot isostatic pressed to homogenize and consolidate the microstructure. The microstructures consisted of grains that were either equiaxed or acicular. In the samples with less carbon loss, the equiaxed grains were either the TaC phase or a TaC matrix that encased fine laths of Ta4C3. In the sample with the most carbon loss, acicular grains were found containing layered and parallel TaC, Ta2C, and Ta4C3 laths along the major-axis of the grains. The phases of the compounds have been determined by using complimentary X-ray diffraction and electron diffraction techniques. Focused ion beam serial sectioning and transmission electron microscopy tilt series tomography were performed to generate three-dimensional reconstructions of the microstructure morphologies. This article addresses how tantalum carbide microstructures are controlled by the overall concentration and phase fraction content in each of these samples.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02811.x" xmlns="http://purl.org/rss/1.0/"><title>Crystallographic Evaluation of Sodium Zirconium Phosphate as a Host Structure for Immobilization of Cesium and Strontium</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02811.x</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Crystallographic Evaluation of Sodium Zirconium Phosphate as a Host Structure for Immobilization of Cesium and Strontium</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ashish Bohre, Om Prakash Shrivastava</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-07-25T14:50:32.168007-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1111/j.1744-7402.2012.02811.x</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1111/j.1744-7402.2012.02811.x</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1111%2Fj.1744-7402.2012.02811.x</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">552</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">563</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Sodium zirconium phosphate (NZP) is a potential material for immobilization of nuclear effluents. It was observed up to ~7.16 wt% (~2.67 mol%) of strontium and ~14.46 wt% (~3.56 mol%) of cesium could be simultaneously loaded into NZP formulations without significant changes in the three-dimensional framework structure. The crystal chemistry of Na<sub>1−<em>x</em></sub>(Cs<sub>1.33</sub>Sr<sub>1</sub>)<sub><em>x</em></sub>Zr<sub>2</sub>P<sub>3</sub>O<sub>12</sub> (<em>x</em> = 0.1–1.0) has been investigated using General Structure Analysis System programming. The CsSrNZP phases crystallize in the space group R-3<em>c</em> and <em>Z</em> = 6. Powder diffraction data have been subjected to Rietveld refinement to arrive at a satisfactory structural convergence of R-factors.</p></div>
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Sodium zirconium phosphate (NZP) is a potential material for immobilization of nuclear effluents. It was observed up to ~7.16 wt% (~2.67 mol%) of strontium and ~14.46 wt% (~3.56 mol%) of cesium could be simultaneously loaded into NZP formulations without significant changes in the three-dimensional framework structure. The crystal chemistry of Na1−x(Cs1.33Sr1)xZr2P3O12 (x = 0.1–1.0) has been investigated using General Structure Analysis System programming. The CsSrNZP phases crystallize in the space group R-3c and Z = 6. Powder diffraction data have been subjected to Rietveld refinement to arrive at a satisfactory structural convergence of R-factors.
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