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            type="text/xsl"?><rdf:RDF xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#"><channel rdf:about="http://onlinelibrary.wiley.com/rss/journal/10.1002/(ISSN)1615-6854" xmlns="http://purl.org/rss/1.0/"><title>Fuel Cells</title><description> Wiley Online Library : Fuel Cells</description><link>http://dx.doi.org/10.1002%2F%28ISSN%291615-6854</link><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc</dc:publisher><dc:language xmlns:dc="http://purl.org/dc/elements/1.1/">en</dc:language><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/">Copyright © 2012 WILEY-VCH Verlag GmbH &amp; Co. KGaA, Weinheim</dc:rights><prism:issn xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1615-6846</prism:issn><prism:eIssn xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1615-6854</prism:eIssn><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><prism:coverDisplayDate xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">December, 2011</prism:coverDisplayDate><prism:volume xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">11</prism:volume><prism:number xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">6</prism:number><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">711</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">931</prism:endingPage><image rdf:resource="http://onlinelibrary.wiley.com/store/10.1002/fuce.v11.6/asset/cover.gif?v=1&amp;s=4f9b8e1f83e7afb5f6c731edaf2d11026f6aba3e"/><items><rdf:Seq><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100047"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100157"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100109"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100095"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100140"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100078"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100105"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100113"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100074"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100107"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100127"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100044"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100058"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100064"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100106"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100116"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100119"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100121"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100126"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100100"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100070"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100051"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100098"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100080"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100079"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100033"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100053"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100042"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201190020"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201190021"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201190018"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201190019"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201000180"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201000182"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201000187"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201000146"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201000148"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201000179"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201000189"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201000167"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201000178"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201000172"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100086"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100090"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100036"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100034"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100025"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100041"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100004"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100017"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100012"/><rdf:li rdf:resource="http://dx.doi.org/10.1002%2Ffuce.201100024"/></rdf:Seq></items></channel><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100047" xmlns="http://purl.org/rss/1.0/"><title>The Error in Gas Temperature Measurements with Thermocouples: Application on an SOFC System Heat Exchanger</title><link>http://dx.doi.org/10.1002%2Ffuce.201100047</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">The Error in Gas Temperature Measurements with Thermocouples: Application on an SOFC System Heat Exchanger</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">L. Tsikonis</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. Van herle</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">D. Favrat</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-02-06T08:42:16.3924-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100047</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/">10.1002/fuce.201100047</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100047</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Aim of this work is to model and study the behavior of thermocouples as they are used in the measurement of gas temperatures in solid oxide fuel cell systems. Due to the high temperature regime in such systems, the effect of radiation and conduction from surrounding solids may bias the measurements with important consequences on control, performance, and cell durability. In order to study these effects a mathematical model of a working thermocouple was developed and it was integrated in that of a heat exchanger, which was part of a larger SOFC system. The enhanced heat exchanger's model was then validated with measurements from a test on a real system. The possibility to overcome the bias and to have a more correct approximation of the real gas temperatures is discussed.</p></div>]]></content:encoded><description>Aim of this work is to model and study the behavior of thermocouples as they are used in the measurement of gas temperatures in solid oxide fuel cell systems. Due to the high temperature regime in such systems, the effect of radiation and conduction from surrounding solids may bias the measurements with important consequences on control, performance, and cell durability. In order to study these effects a mathematical model of a working thermocouple was developed and it was integrated in that of a heat exchanger, which was part of a larger SOFC system. The enhanced heat exchanger's model was then validated with measurements from a test on a real system. The possibility to overcome the bias and to have a more correct approximation of the real gas temperatures is discussed.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100157" xmlns="http://purl.org/rss/1.0/"><title>Reaction Kinetics of Hydroxyl Radicals with Model Compounds of Fuel Cell Polymer Membranes</title><link>http://dx.doi.org/10.1002%2Ffuce.201100157</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Reaction Kinetics of Hydroxyl Radicals with Model Compounds of Fuel Cell Polymer Membranes</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A. M. Dreizler</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">E. Roduner</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-02-02T02:30:24.366214-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100157</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/">10.1002/fuce.201100157</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100157</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The chemical stability of perfluorinated and non-perfluorinated low temperature fuel cell model compounds (MCs) against attack by hydroxyl radicals, HO<sup>•</sup>, is compared using a competition kinetics approach in aqueous solutions at ambient temperature. HO<sup>•</sup> radicals were generated <em>in situ</em> by UV photolysis of hydrogen peroxide in the electron spin resonance (ESR) resonator. Acetic acid (AA), trifluoroacetic acid (TFAA), methanesulfonic acid (MSA), trifluorosulfonic acid (TFSA), and perfluoro(2-ethoxyethane)sulfonic acid (PFEESA) were chosen as MCs, while the rate constants of 5,5-dimethyl-1-pyrroline-<em>N</em>-oxide (DMPO) and methanol (CH<sub>3</sub>OH) served as reference for the determination of relative rate constants by means of steady state ESR signal amplitudes. In decreasing order the rate constants are: <em>k</em><sub>MSA</sub> = (4.8 ± 0.2) × 10<sup>7</sup> M<sup>–1</sup> s<sup>–1</sup>, <em>k</em><sub>AA</sub> = (4.2 ± 0.3) × 10<sup>7</sup> M<sup>–1</sup> s<sup>–1</sup>, <em>k</em><sub>PFEESA</sub> = (3.7 ± 0.1) × 10<sup>6</sup> M<sup>–1</sup> s<sup>–1</sup>, <em>k</em><sub>TFAA</sub> = (7.9 ± 0.2) × 10<sup>5</sup> M<sup>–1</sup> s<sup>–1</sup>, and <em>k</em><sub>TFSA</sub> &lt; 1.0 × 10<sup>5</sup> M<sup>–1</sup> s<sup>–1</sup>. Applying these results to perfluorinated fuel cell membranes like Nafion®, the main points of attack by HO<sup>•</sup> are concluded to be the ether groups of the side chains, followed by the remaining carboxyl groups from the manufacturing process of the polymers.</p></div>]]></content:encoded><description>The chemical stability of perfluorinated and non-perfluorinated low temperature fuel cell model compounds (MCs) against attack by hydroxyl radicals, HO•, is compared using a competition kinetics approach in aqueous solutions at ambient temperature. HO• radicals were generated in situ by UV photolysis of hydrogen peroxide in the electron spin resonance (ESR) resonator. Acetic acid (AA), trifluoroacetic acid (TFAA), methanesulfonic acid (MSA), trifluorosulfonic acid (TFSA), and perfluoro(2-ethoxyethane)sulfonic acid (PFEESA) were chosen as MCs, while the rate constants of 5,5-dimethyl-1-pyrroline-N-oxide (DMPO) and methanol (CH3OH) served as reference for the determination of relative rate constants by means of steady state ESR signal amplitudes. In decreasing order the rate constants are: kMSA = (4.8 ± 0.2) × 107 M–1 s–1, kAA = (4.2 ± 0.3) × 107 M–1 s–1, kPFEESA = (3.7 ± 0.1) × 106 M–1 s–1, kTFAA = (7.9 ± 0.2) × 105 M–1 s–1, and kTFSA &lt; 1.0 × 105 M–1 s–1. Applying these results to perfluorinated fuel cell membranes like Nafion®, the main points of attack by HO• are concluded to be the ether groups of the side chains, followed by the remaining carboxyl groups from the manufacturing process of the polymers.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100109" xmlns="http://purl.org/rss/1.0/"><title>A Performance Study of Solid Oxide Fuel Cells With BaZr0.1Ce0.7Y0.2O3–δ Electrolyte Developed by Spray-Modified Pressing Method</title><link>http://dx.doi.org/10.1002%2Ffuce.201100109</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A Performance Study of Solid Oxide Fuel Cells With BaZr0.1Ce0.7Y0.2O3–δ Electrolyte Developed by Spray-Modified Pressing Method</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">B. Guan</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Z. Lü</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">G. Wang</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">B. Wei</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">W. Li</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">X. Huang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-02-02T02:30:22.657978-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100109</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/">10.1002/fuce.201100109</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100109</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Fuel cells with BaZr<sub>0.1</sub>Ce<sub>0.7</sub>Y<sub>0.2</sub>O<sub>3–δ</sub> (BZCY) proton-conducting electrolyte is fabricated using spray-modified pressing method. In the present study the spray-modified pressing technology is developed to prepare thin electrolyte layers on porous Ni-BZCY anode supports. SEM data show the BZCY electrolyte film is uniform and dense, well-bonded with the anode substrate. An anode-supported fuel cell with BZCY electrolyte and Ba<sub>0.5</sub>Sr<sub>0.5</sub>Co<sub>0.8</sub>Fe<sub>0.2</sub>O<sub>3–δ</sub> (BSCF) cathode is characterized from 600 to 700 °C using hydrogen as fuel and ambient air as oxidant. Maximum power density of 536 mW cm<sup>–2</sup> along with a 1.01 V OCV at 700 °C is obtained. Impedance spectra show that Ohmic resistances contribute minor parts to the total ones, for instance, only ~23% when operating at 600 °C. The results demonstrate that spray-modified pressing technology offers a simple and effective way to fabricate quality electrolyte film suitable to operate in intermediate temperature.</p></div>]]></content:encoded><description>Fuel cells with BaZr0.1Ce0.7Y0.2O3–δ (BZCY) proton-conducting electrolyte is fabricated using spray-modified pressing method. In the present study the spray-modified pressing technology is developed to prepare thin electrolyte layers on porous Ni-BZCY anode supports. SEM data show the BZCY electrolyte film is uniform and dense, well-bonded with the anode substrate. An anode-supported fuel cell with BZCY electrolyte and Ba0.5Sr0.5Co0.8Fe0.2O3–δ (BSCF) cathode is characterized from 600 to 700 °C using hydrogen as fuel and ambient air as oxidant. Maximum power density of 536 mW cm–2 along with a 1.01 V OCV at 700 °C is obtained. Impedance spectra show that Ohmic resistances contribute minor parts to the total ones, for instance, only ~23% when operating at 600 °C. The results demonstrate that spray-modified pressing technology offers a simple and effective way to fabricate quality electrolyte film suitable to operate in intermediate temperature.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100095" xmlns="http://purl.org/rss/1.0/"><title>Modeling of Solid Oxide Fuel Cells with Particle Size and Porosity Grading in Anode Electrode</title><link>http://dx.doi.org/10.1002%2Ffuce.201100095</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Modeling of Solid Oxide Fuel Cells with Particle Size and Porosity Grading in Anode Electrode</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">L. Liu</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">R. Flesner</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">G.-Y. Kim</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A. Chandra</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-02-02T02:30:21.373559-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100095</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/">10.1002/fuce.201100095</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100095</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Solid oxide fuel cells (SOFCs) have the potential to meet the critical energy needs of our modern civilization and minimize the adverse environmental impacts from excessive energy consumption. They are highly efficient, clean, and can run on variety of fuel gases. However, little investigative focus has been put on optimal power output based on electrode microstructure. In this work, a complete electrode polarization model of SOFCs has been developed and utilized to analyze the performance of functionally graded anode with different particle size and porosity profiles. The model helps to understand the implications of varying the electrode microstructure from the polarization standpoint. The work identified conditions when grading can improve the cell performance and showed that grading is not always beneficial or necessary.</p></div>]]></content:encoded><description>Solid oxide fuel cells (SOFCs) have the potential to meet the critical energy needs of our modern civilization and minimize the adverse environmental impacts from excessive energy consumption. They are highly efficient, clean, and can run on variety of fuel gases. However, little investigative focus has been put on optimal power output based on electrode microstructure. In this work, a complete electrode polarization model of SOFCs has been developed and utilized to analyze the performance of functionally graded anode with different particle size and porosity profiles. The model helps to understand the implications of varying the electrode microstructure from the polarization standpoint. The work identified conditions when grading can improve the cell performance and showed that grading is not always beneficial or necessary.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100140" xmlns="http://purl.org/rss/1.0/"><title>Modeling and Optimization of Anode-Supported Solid Oxide Fuel Cells on Cell Parameters via Artificial Neural Network and Genetic Algorithm</title><link>http://dx.doi.org/10.1002%2Ffuce.201100140</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Modeling and Optimization of Anode-Supported Solid Oxide Fuel Cells on Cell Parameters via Artificial Neural Network and Genetic Algorithm</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Bozorgmehri</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. Hamedi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-25T05:11:00.520016-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100140</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/">10.1002/fuce.201100140</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100140</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>An artificial neural network (ANN) and a genetic algorithm (GA) are employed to model and optimize cell parameters to improve the performance of singular, intermediate-temperature, solid oxide fuel cells (IT-SOFCs). The ANN model uses a feed-forward neural network with an error back-propagation algorithm. The ANN is trained using experimental data as a black-box without using physical models. The developed model is able to predict the performance of the SOFC. An optimization algorithm is utilized to select the optimal SOFC parameters. The optimal values of four cell parameters (anode support thickness, anode support porosity, electrolyte thickness, and functional layer cathode thickness) are determined by using the GA under different conditions. The results show that these optimum cell parameters deliver the highest maximum power density under different constraints on the anode support thickness, porosity, and electrolyte thickness.</p></div>]]></content:encoded><description>An artificial neural network (ANN) and a genetic algorithm (GA) are employed to model and optimize cell parameters to improve the performance of singular, intermediate-temperature, solid oxide fuel cells (IT-SOFCs). The ANN model uses a feed-forward neural network with an error back-propagation algorithm. The ANN is trained using experimental data as a black-box without using physical models. The developed model is able to predict the performance of the SOFC. An optimization algorithm is utilized to select the optimal SOFC parameters. The optimal values of four cell parameters (anode support thickness, anode support porosity, electrolyte thickness, and functional layer cathode thickness) are determined by using the GA under different conditions. The results show that these optimum cell parameters deliver the highest maximum power density under different constraints on the anode support thickness, porosity, and electrolyte thickness.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100078" xmlns="http://purl.org/rss/1.0/"><title>A New Stack to Validate Technical Solutions and Numerical Simulations</title><link>http://dx.doi.org/10.1002%2Ffuce.201100078</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A New Stack to Validate Technical Solutions and Numerical Simulations</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">T. Boëdec</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. Reytier</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">D. Lhachemi</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">D. Tschumperlé</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">P. Louat</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Di Iorio</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">P. Baurens</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">G. Delette</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-25T05:10:59.206771-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100078</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/">10.1002/fuce.201100078</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100078</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>A new design of High Temperature Steam Electrolyzer (HTSE) based on metallic seals, associated to an insulating cell support and a flexible interconnect system has been proposed. In this work, complete simulations of this 3D design have been performed with ANSYS®-FLUENT® software. The temperature repartition is determined by taking into account thermal exchanges, fluids movements, and electrochemical reactions. Moreover, due to stress relaxation mechanism, the flexible interconnect loading decreases during time, which may impact the contact resistance and the electrochemical solution. A possible degradation of the contact resistance with time is predicted by the simulation and its effect will be discussed according to some design parameters. Steam electrolysis tests have been conducted at 800 °C on this new design. The comparisons to the simulations are also presented. All these results obtained in this study lead to propose some recommendations for such a design.</p></div>]]></content:encoded><description>A new design of High Temperature Steam Electrolyzer (HTSE) based on metallic seals, associated to an insulating cell support and a flexible interconnect system has been proposed. In this work, complete simulations of this 3D design have been performed with ANSYS®-FLUENT® software. The temperature repartition is determined by taking into account thermal exchanges, fluids movements, and electrochemical reactions. Moreover, due to stress relaxation mechanism, the flexible interconnect loading decreases during time, which may impact the contact resistance and the electrochemical solution. A possible degradation of the contact resistance with time is predicted by the simulation and its effect will be discussed according to some design parameters. Steam electrolysis tests have been conducted at 800 °C on this new design. The comparisons to the simulations are also presented. All these results obtained in this study lead to propose some recommendations for such a design.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100105" xmlns="http://purl.org/rss/1.0/"><title>Preparation of Platinum-Poly(O-dihydroxybenzene) Composite Catalyst and Its Electrocatalytic Activity Toward Methanol and Formic Acid Oxidation</title><link>http://dx.doi.org/10.1002%2Ffuce.201100105</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Preparation of Platinum-Poly(O-dihydroxybenzene) Composite Catalyst and Its Electrocatalytic Activity Toward Methanol and Formic Acid Oxidation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">F. Ren</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">R. Zhou</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">F. Jiang</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">W. Zhou</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Y. Du</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. Xu</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">C. Wang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-23T08:12:01.663913-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100105</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/">10.1002/fuce.201100105</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100105</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>A composite catalyst has been successfully prepared by dispersing Pt nanoparticles on a poly(<em>o</em>-dihydroxybenzene) (P<em>o</em>DHB) modified glassy carbon (GC) electrode and characterized by SEM, EDX, and electrochemical analysis. Compared with Pt nanoparticles deposited on the bare GC, the Pt/P<em>o</em>DHB/GC exhibits higher catalytic activity and stronger poisoning tolerance for electro-oxidation of methanol and formic acid. The enhanced performance could be attributed to the increase of electrochemical active surface area (EASA) arisen from the P<em>o</em>DHB modification. Furthermore, performance limiting factors such as platinum loading, polymer mass, H<sub>2</sub>SO<sub>4</sub>, methanol, and formic acid concentrations have been evaluated for optimizing the electrocatalytic activities.</p></div>]]></content:encoded><description>A composite catalyst has been successfully prepared by dispersing Pt nanoparticles on a poly(o-dihydroxybenzene) (PoDHB) modified glassy carbon (GC) electrode and characterized by SEM, EDX, and electrochemical analysis. Compared with Pt nanoparticles deposited on the bare GC, the Pt/PoDHB/GC exhibits higher catalytic activity and stronger poisoning tolerance for electro-oxidation of methanol and formic acid. The enhanced performance could be attributed to the increase of electrochemical active surface area (EASA) arisen from the PoDHB modification. Furthermore, performance limiting factors such as platinum loading, polymer mass, H2SO4, methanol, and formic acid concentrations have been evaluated for optimizing the electrocatalytic activities.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100113" xmlns="http://purl.org/rss/1.0/"><title>Durable Transition-Metal-Carbide-Supported Pt–Ru Anodes for Direct Methanol Fuel Cells</title><link>http://dx.doi.org/10.1002%2Ffuce.201100113</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Durable Transition-Metal-Carbide-Supported Pt–Ru Anodes for Direct Methanol Fuel Cells</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">K. G. Nishanth</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">P. Sridhar</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Pitchumani</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A. K. Shukla</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-13T06:53:35.008899-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100113</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/">10.1002/fuce.201100113</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100113</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Molybdenum carbide (MoC) and tungsten carbide (WC) are synthesized by direct carbonization method. Pt–Ru catalysts supported on MoC, WC, and Vulcan XC-72R are prepared, and characterized by X-ray diffraction, X-ray photoelectron spectroscopy, and transmission electron microscopy in conjunction with electrochemistry. Electrochemical activities for the catalysts towards methanol electro-oxidation are studied by cyclic voltammetry. All the electro-catalysts are subjected to accelerated durability test (ADT). The electrochemical activity of carbide-supported electro-catalysts towards methanol electro-oxidation is found to be higher than carbon-supported catalysts before and after ADT. The study suggests that Pt–Ru/MoC and Pt–Ru/WC catalysts are more durable than Pt–Ru/C. Direct methanol fuel cells (DMFCs) with Pt–Ru/MoC and Pt–Ru/WC anodes also exhibit higher performance than the DMFC with Pt–Ru/C anode.</p></div>]]></content:encoded><description>Molybdenum carbide (MoC) and tungsten carbide (WC) are synthesized by direct carbonization method. Pt–Ru catalysts supported on MoC, WC, and Vulcan XC-72R are prepared, and characterized by X-ray diffraction, X-ray photoelectron spectroscopy, and transmission electron microscopy in conjunction with electrochemistry. Electrochemical activities for the catalysts towards methanol electro-oxidation are studied by cyclic voltammetry. All the electro-catalysts are subjected to accelerated durability test (ADT). The electrochemical activity of carbide-supported electro-catalysts towards methanol electro-oxidation is found to be higher than carbon-supported catalysts before and after ADT. The study suggests that Pt–Ru/MoC and Pt–Ru/WC catalysts are more durable than Pt–Ru/C. Direct methanol fuel cells (DMFCs) with Pt–Ru/MoC and Pt–Ru/WC anodes also exhibit higher performance than the DMFC with Pt–Ru/C anode.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100074" xmlns="http://purl.org/rss/1.0/"><title>Design and Optimization of Composite Electrodes in Solid Oxide Cells</title><link>http://dx.doi.org/10.1002%2Ffuce.201100074</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Design and Optimization of Composite Electrodes in Solid Oxide Cells</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">X.-M. Ge</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Y.-N. Fang</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S.-H. Chan</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-13T06:53:34.066104-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100074</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/">10.1002/fuce.201100074</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100074</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The performance of solid oxide cells (SOCs) heavily relies on the population of three-phase boundaries (TPBs) in the composite electrodes. In this study, SOC composite electrodes are described by percolating binary particle aggregates that are constructed from random loose packing models and classical sintering theories. Summed perimeters of the sintering necks represent the total TPB lengths. A case study has been carried out on lanthanum strontium manganite (LSM)–yttria-stabilized zirconia (YSZ) composite electrodes. By employing three-dimensional data that are converted from relevant two-dimensional data, the TPB length of baseline LSM–YSZ electrodes investigated in this study is 35.4 μm μm<sup>–3</sup>. The parametric and sensitivity analyses show the changes of TPB lengths in functions of the weight fraction of powders, particle size and particle size ratio of powders, void fraction of electrodes, and density of materials. In the case of baseline LSM–YSZ electrodes, proper electrode design and optimization would result in 2–3 times of the enlargement of TPBs. Technical guidelines on the design and optimization of SOC composite electrodes are proposed.</p></div>]]></content:encoded><description>The performance of solid oxide cells (SOCs) heavily relies on the population of three-phase boundaries (TPBs) in the composite electrodes. In this study, SOC composite electrodes are described by percolating binary particle aggregates that are constructed from random loose packing models and classical sintering theories. Summed perimeters of the sintering necks represent the total TPB lengths. A case study has been carried out on lanthanum strontium manganite (LSM)–yttria-stabilized zirconia (YSZ) composite electrodes. By employing three-dimensional data that are converted from relevant two-dimensional data, the TPB length of baseline LSM–YSZ electrodes investigated in this study is 35.4 μm μm–3. The parametric and sensitivity analyses show the changes of TPB lengths in functions of the weight fraction of powders, particle size and particle size ratio of powders, void fraction of electrodes, and density of materials. In the case of baseline LSM–YSZ electrodes, proper electrode design and optimization would result in 2–3 times of the enlargement of TPBs. Technical guidelines on the design and optimization of SOC composite electrodes are proposed.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100107" xmlns="http://purl.org/rss/1.0/"><title>Proton Conducting Membranes Based on Poly(2,2′-imidazole-5,5′-bibenzimidazole)</title><link>http://dx.doi.org/10.1002%2Ffuce.201100107</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Proton Conducting Membranes Based on Poly(2,2′-imidazole-5,5′-bibenzimidazole)</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Y. Guan</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">H. Pu</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. Jin</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Z. Chang</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A. D. Modestov</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-13T06:53:33.019239-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100107</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/">10.1002/fuce.201100107</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100107</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Poly(2,2′-imidazole-5,5′-bibenzimidazole) (PBI-imi) was synthesized via the polycondensation between 3,3′,4,4′-tetraaminobiphenyl and 4,5-imidazole-dicarboxylic acid. Effects of the reaction conditions on the intrinsic viscosity of the synthesized polymers were studied. The results show that the molecular weight of the polymers increases with increasing monomer concentration and reaction time, and then levels off. With higher reaction temperature, the molecular weight of the polymer is higher. With the additional imidazole group in the backbone, PBI-imi shows improved phosphoric acid doping ability, as well as a little higher proton conductivity when compared with widely used poly[2,2′-(m-phenylene)-5,5′-bibenzimidazole] (PBI-ph).Whereas, PBI-imi and PBI-ph have the similar chemical oxidation stability. PBI-imi/3.0 H<sub>3</sub>PO<sub>4</sub> composite membranes exhibit a proton conductivity as high as 10<sup>–4</sup> S cm<sup>–1</sup> at 150 °C under anhydrous condition. The temperature dependence of proton conductivity of acid doped PBI-imi can be modeled by an Arrhenius equation.</p></div>]]></content:encoded><description>Poly(2,2′-imidazole-5,5′-bibenzimidazole) (PBI-imi) was synthesized via the polycondensation between 3,3′,4,4′-tetraaminobiphenyl and 4,5-imidazole-dicarboxylic acid. Effects of the reaction conditions on the intrinsic viscosity of the synthesized polymers were studied. The results show that the molecular weight of the polymers increases with increasing monomer concentration and reaction time, and then levels off. With higher reaction temperature, the molecular weight of the polymer is higher. With the additional imidazole group in the backbone, PBI-imi shows improved phosphoric acid doping ability, as well as a little higher proton conductivity when compared with widely used poly[2,2′-(m-phenylene)-5,5′-bibenzimidazole] (PBI-ph).Whereas, PBI-imi and PBI-ph have the similar chemical oxidation stability. PBI-imi/3.0 H3PO4 composite membranes exhibit a proton conductivity as high as 10–4 S cm–1 at 150 °C under anhydrous condition. The temperature dependence of proton conductivity of acid doped PBI-imi can be modeled by an Arrhenius equation.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100127" xmlns="http://purl.org/rss/1.0/"><title>Temperature Measurement and Distribution Inside Planar SOFC Stacks</title><link>http://dx.doi.org/10.1002%2Ffuce.201100127</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Temperature Measurement and Distribution Inside Planar SOFC Stacks</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">W. B. Guan</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">H. J. Zhai</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">L. Jin</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">C. Xu</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">W. G. Wang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-13T06:34:48.799044-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100127</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/">10.1002/fuce.201100127</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100127</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>In this work, a kind of thin K-type thermocouple and self-developed CAS-I sealant were used to assembly solid oxide fuel cell (SOFC) stacks and temperatures of unit cells inside a planar SOFC stack were measured. The open circuit voltage testing of the stack and characterization of the interface between sealant and components suggested excellent sealing effect by applying the developed method. The effect of discharging direct-current on temperature and temperature distribution inside the designed SOFC stack was investigated. The results showed that the discharging current had a great impact and the gas flow rate had a slight impact on the temperatures of unit cells. Temperature distribution of unit cells inside the stack was much non-uniform and there is a significant temperature difference between various components of the stack and heating environment. The relationship between temperatures and cell performance showed that the worse the cell performance, the higher the cell surface temperature. When the stack was discharged at a constant current and the temperature of cell surface was over 950 °C, the higher the temperature, the more drop the corresponding voltage.</p></div>]]></content:encoded><description>In this work, a kind of thin K-type thermocouple and self-developed CAS-I sealant were used to assembly solid oxide fuel cell (SOFC) stacks and temperatures of unit cells inside a planar SOFC stack were measured. The open circuit voltage testing of the stack and characterization of the interface between sealant and components suggested excellent sealing effect by applying the developed method. The effect of discharging direct-current on temperature and temperature distribution inside the designed SOFC stack was investigated. The results showed that the discharging current had a great impact and the gas flow rate had a slight impact on the temperatures of unit cells. Temperature distribution of unit cells inside the stack was much non-uniform and there is a significant temperature difference between various components of the stack and heating environment. The relationship between temperatures and cell performance showed that the worse the cell performance, the higher the cell surface temperature. When the stack was discharged at a constant current and the temperature of cell surface was over 950 °C, the higher the temperature, the more drop the corresponding voltage.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100044" xmlns="http://purl.org/rss/1.0/"><title>Alcohol Crossover Behavior in Direct Alcohol Fuel Cells (DAFCs) System</title><link>http://dx.doi.org/10.1002%2Ffuce.201100044</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Alcohol Crossover Behavior in Direct Alcohol Fuel Cells (DAFCs) System</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Y. H. Chu</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Y. G. Shul</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-13T06:34:47.664199-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100044</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/">10.1002/fuce.201100044</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100044</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The alcohols (methanol, ethanol, and 1-propanol) crossover behavior of through fuel cell membrane electrode assembly (MEA) in direct alcohol fuel cell (DAFC) system was studied. We divided five different factors which affect alcohol crossover behavior through MEA to analyze alcohol crossover behavior. Those are membrane effect, physical blocking effect of anode, alcohol oxidation effect of anode electrocatalysts, physical blocking effect of cathode, and alcohol oxidation effect of cathode. Among these five factors, the four factors caused by two different electrodes (anode and cathode) were evaluated by fabricating various types of MEA. In the case of alcohols through membrane without any electrode was increased when the cell temperature was raised from room temperature to 100 °C, but it was decreased above the cell temperature of 100 °C. Among the electrode effects on alcohol crossover rate, physical blocking effect of electrodes played dominant role below 100 °C. However alcohol oxidation effects of electrodes was predominant above the 100 °C.</p></div>]]></content:encoded><description>The alcohols (methanol, ethanol, and 1-propanol) crossover behavior of through fuel cell membrane electrode assembly (MEA) in direct alcohol fuel cell (DAFC) system was studied. We divided five different factors which affect alcohol crossover behavior through MEA to analyze alcohol crossover behavior. Those are membrane effect, physical blocking effect of anode, alcohol oxidation effect of anode electrocatalysts, physical blocking effect of cathode, and alcohol oxidation effect of cathode. Among these five factors, the four factors caused by two different electrodes (anode and cathode) were evaluated by fabricating various types of MEA. In the case of alcohols through membrane without any electrode was increased when the cell temperature was raised from room temperature to 100 °C, but it was decreased above the cell temperature of 100 °C. Among the electrode effects on alcohol crossover rate, physical blocking effect of electrodes played dominant role below 100 °C. However alcohol oxidation effects of electrodes was predominant above the 100 °C.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100058" xmlns="http://purl.org/rss/1.0/"><title>Influence of Microwave-Assisted Pechini Method on La0.80Sr0.20Ga0.83Mg0.17O3–δ Ionic Conductivity</title><link>http://dx.doi.org/10.1002%2Ffuce.201100058</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Influence of Microwave-Assisted Pechini Method on La0.80Sr0.20Ga0.83Mg0.17O3–δ Ionic Conductivity</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Boldrini</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">C. Mortalò</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Fasolin</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">F. Agresti</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">L. Doubova</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. Fabrizio</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">and S. Barison</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-13T06:34:41.754512-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100058</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/">10.1002/fuce.201100058</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100058</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>With the aim of investigating the microwave influence on the electrolyte material properties, La<sub>0.80</sub>Sr<sub>0.20</sub>Ga<sub>0.83</sub>Mg<sub>0.17</sub>O<sub>2.815</sub> was prepared by both a conventional and a microwave-assisted sol–gel Pechini method. With respect to the conventional Pechini method (hereafter SGP), the microwave assisted process (hereafter MWA-SGP) guaranteed a faster procedure, reducing the time needed to remove the excess solvents to complete the polyesterification reaction from some days to a few hours. In fact, when a MWA-SGP method was used, powders having higher phase purity were obtained. The sintering process at 1,450 °C of the powders prepared by both methods yielded pellets with similar density values (≥92% of theoretical). Nevertheless, only by microwave-assisted process single-phase products were obtained and no secondary phases such as tetragonal LaSrGaO<sub>4</sub> and LaSrGa<sub>3</sub>O<sub>7</sub> were detected. These by-products have been demonstrated to be detrimental for conductivity. Indeed, pellets obtained by MWA-SGP method showed oxygen ionic conductivity values higher (about 30–40%) than those checked for SGP samples, thus demonstrating the important role of the microwave process on reducing time and costs and on improving the electrolyte properties.</p></div>]]></content:encoded><description>With the aim of investigating the microwave influence on the electrolyte material properties, La0.80Sr0.20Ga0.83Mg0.17O2.815 was prepared by both a conventional and a microwave-assisted sol–gel Pechini method. With respect to the conventional Pechini method (hereafter SGP), the microwave assisted process (hereafter MWA-SGP) guaranteed a faster procedure, reducing the time needed to remove the excess solvents to complete the polyesterification reaction from some days to a few hours. In fact, when a MWA-SGP method was used, powders having higher phase purity were obtained. The sintering process at 1,450 °C of the powders prepared by both methods yielded pellets with similar density values (≥92% of theoretical). Nevertheless, only by microwave-assisted process single-phase products were obtained and no secondary phases such as tetragonal LaSrGaO4 and LaSrGa3O7 were detected. These by-products have been demonstrated to be detrimental for conductivity. Indeed, pellets obtained by MWA-SGP method showed oxygen ionic conductivity values higher (about 30–40%) than those checked for SGP samples, thus demonstrating the important role of the microwave process on reducing time and costs and on improving the electrolyte properties.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100064" xmlns="http://purl.org/rss/1.0/"><title>Characterization and Comparison of Different Cathode Materials for SC-SOFC: LSM, BSCF, SSC, and LSCF</title><link>http://dx.doi.org/10.1002%2Ffuce.201100064</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Characterization and Comparison of Different Cathode Materials for SC-SOFC: LSM, BSCF, SSC, and LSCF</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">D. Rembelski</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. P. Viricelle</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">L. Combemale</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. Rieu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-13T06:34:35.862503-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100064</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/">10.1002/fuce.201100064</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100064</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Four cathode materials for single chamber solid oxide fuel cell (SC-SOFC) [La<sub>0.8</sub>Sr<sub>0.2</sub>MnO<sub>3–δ</sub> (LSM), Ba<sub>0.5</sub>Sr<sub>0.5</sub>Co<sub>0.8</sub>Fe<sub>0.2</sub>O<sub>3–δ</sub> (BSCF), Sm<sub>0.5</sub>Sr<sub>0.5</sub>CoO<sub>3–δ</sub> (SSC), and La<sub>0.6</sub>Sr<sub>0.4</sub>Co<sub>0.2</sub>Fe<sub>0.8</sub>O<sub>3–δ</sub> (LSCF)] were investigated regarding their chemical stability, electrical conductivity, catalytic activity, and polarization resistance under air and methane/air atmosphere. Electrolyte-supported fuel cells, with Ce<sub>0.9</sub>Gd<sub>0.1</sub>O<sub>2–δ</sub> (CGO) electrolyte and a Ni-CGO anode, were tested in several methane/air mixtures with each cathode materials between 625 and 725 °C. These single cells were not optimized but only designed to compare the four studied cathodes. The decrease of methane-to-oxygen ratio from 2 to 0.67 strongly increased the performance of fuel cells for all cathode materials but the effect of temperature was not always significant. Cells with SSC, BSCF, and LSCF have shown a maximum power density about 20 mW cm<sup>–2</sup> while the cell with LSM has given only 5 mW cm<sup>–2</sup>.</p></div>]]></content:encoded><description>Four cathode materials for single chamber solid oxide fuel cell (SC-SOFC) [La0.8Sr0.2MnO3–δ (LSM), Ba0.5Sr0.5Co0.8Fe0.2O3–δ (BSCF), Sm0.5Sr0.5CoO3–δ (SSC), and La0.6Sr0.4Co0.2Fe0.8O3–δ (LSCF)] were investigated regarding their chemical stability, electrical conductivity, catalytic activity, and polarization resistance under air and methane/air atmosphere. Electrolyte-supported fuel cells, with Ce0.9Gd0.1O2–δ (CGO) electrolyte and a Ni-CGO anode, were tested in several methane/air mixtures with each cathode materials between 625 and 725 °C. These single cells were not optimized but only designed to compare the four studied cathodes. The decrease of methane-to-oxygen ratio from 2 to 0.67 strongly increased the performance of fuel cells for all cathode materials but the effect of temperature was not always significant. Cells with SSC, BSCF, and LSCF have shown a maximum power density about 20 mW cm–2 while the cell with LSM has given only 5 mW cm–2.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100106" xmlns="http://purl.org/rss/1.0/"><title>Characterization of La0.6Sr0.4Co0.2Fe0.8O3–δ + La2NiO4+δ Composite Cathode Materials for Solid Oxide Fuel Cells</title><link>http://dx.doi.org/10.1002%2Ffuce.201100106</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Characterization of La0.6Sr0.4Co0.2Fe0.8O3–δ + La2NiO4+δ Composite Cathode Materials for Solid Oxide Fuel Cells</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. Chen</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">B. H. Moon</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. H. Kim</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">B. H. Kim</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Q. Xu</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">B.-G. Ahn</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-13T06:34:28.782875-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100106</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/">10.1002/fuce.201100106</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100106</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The structure, electrical conduction, thermal expansion and electrochemical properties of the La<sub>0.6</sub>Sr<sub>0.4</sub>Co<sub>0.2</sub>Fe<sub>0.8</sub>O<sub>3–δ</sub> + La<sub>2</sub>NiO<sub>4+δ</sub> (LSCF-LNO) composite cathodes were investigated with regard to the volume fraction of the LNO composition. No chemical reaction product between the two constituent phases was found for the composite cathodes sintered at 1,400 °C for 10 h within the sensitivity of the XRD. Compared to the performance of the LSCF cathode, the LNO composition in the composite cathode plays a role in deteriorating both electrical conductivity and electrochemical properties, however, improving the thermal expansion properties. The trade-off between electrical conducting and thermal expansion classifies the composite cathode containing 30 volume percent (vol.%) LNO as the optimum composition. For characterizing cathode performance in a single cell, a slurry spin coating technique was employed to prepare a porous cathode layer as well as a YSZ/Ce<sub>0.8</sub>Sm<sub>0.2</sub>O<sub>3–δ</sub> (SDC) electrolyte. The optimum conditions for fabricating the YSZ/SDC electrolyte were investigated. The resulting single cell with 70 vol.% LSCF-30 vol.%LNO (LSCF-LNO30) cathode shows a power density of 497 mW cm<sup>–2</sup> at 800 °C, which is lower than that of the cell with a LSCF cathode, but still within the limits acceptable for practical applications.</p></div>]]></content:encoded><description>The structure, electrical conduction, thermal expansion and electrochemical properties of the La0.6Sr0.4Co0.2Fe0.8O3–δ + La2NiO4+δ (LSCF-LNO) composite cathodes were investigated with regard to the volume fraction of the LNO composition. No chemical reaction product between the two constituent phases was found for the composite cathodes sintered at 1,400 °C for 10 h within the sensitivity of the XRD. Compared to the performance of the LSCF cathode, the LNO composition in the composite cathode plays a role in deteriorating both electrical conductivity and electrochemical properties, however, improving the thermal expansion properties. The trade-off between electrical conducting and thermal expansion classifies the composite cathode containing 30 volume percent (vol.%) LNO as the optimum composition. For characterizing cathode performance in a single cell, a slurry spin coating technique was employed to prepare a porous cathode layer as well as a YSZ/Ce0.8Sm0.2O3–δ (SDC) electrolyte. The optimum conditions for fabricating the YSZ/SDC electrolyte were investigated. The resulting single cell with 70 vol.% LSCF-30 vol.%LNO (LSCF-LNO30) cathode shows a power density of 497 mW cm–2 at 800 °C, which is lower than that of the cell with a LSCF cathode, but still within the limits acceptable for practical applications.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100116" xmlns="http://purl.org/rss/1.0/"><title>Flexural Strength and Viscosity of Glass Ceramic Sealants for Solid Oxide Fuel Cell Stacks</title><link>http://dx.doi.org/10.1002%2Ffuce.201100116</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Flexural Strength and Viscosity of Glass Ceramic Sealants for Solid Oxide Fuel Cell Stacks</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. Malzbender</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Y. Zhao</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-13T06:34:21.207413-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100116</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/">10.1002/fuce.201100116</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100116</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The structural integrity of the sealing material is critical for the reliability of solid oxide fuel cell stacks. In this respect failure and deformation are aspects which need to be assessed in particular for glass ceramic sealant materials. Bending tests were carried at room temperature and typical stack operation temperature for glass ceramic sealants with different crystallization levels. Elastic moduli, fracture stresses, and viscosity values are reported. In addition to sintered bars some bending testing were carried out for steel specimens that were head-to-head joined with the glass ceramics similar as in a stack application. The ceramic particle reinforced sealant material was screen printed onto the steel. The results reveal a decrease of the strength for the partially crystallized sealant at operation relevant temperatures that can be associated with the viscous deformation of the material.</p></div>]]></content:encoded><description>The structural integrity of the sealing material is critical for the reliability of solid oxide fuel cell stacks. In this respect failure and deformation are aspects which need to be assessed in particular for glass ceramic sealant materials. Bending tests were carried at room temperature and typical stack operation temperature for glass ceramic sealants with different crystallization levels. Elastic moduli, fracture stresses, and viscosity values are reported. In addition to sintered bars some bending testing were carried out for steel specimens that were head-to-head joined with the glass ceramics similar as in a stack application. The ceramic particle reinforced sealant material was screen printed onto the steel. The results reveal a decrease of the strength for the partially crystallized sealant at operation relevant temperatures that can be associated with the viscous deformation of the material.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100119" xmlns="http://purl.org/rss/1.0/"><title>Study of a Single-Chamber Solid Oxide Fuel Cell Microstack with V-Shaped Congener-Electrode-Facing Configuration</title><link>http://dx.doi.org/10.1002%2Ffuce.201100119</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Study of a Single-Chamber Solid Oxide Fuel Cell Microstack with V-Shaped Congener-Electrode-Facing Configuration</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Y. Tian</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Z. Lü</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Y. Zhang</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">B. Wei</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. Liu</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">X. Huang</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">W. Su</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-13T06:34:20.027653-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100119</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/">10.1002/fuce.201100119</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100119</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Single-chamber solid oxide fuel cell (SC-SOFC) microstacks with V-Shaped congener-electrode-facing configuration were fabricated and operated successfully in a box-like stainless steel chamber. Two gas channels with small gas inlets were used to transport the fuel and oxygen to the anodes and cathodes, respectively. The temperature of an anode-facing-anode two-cell stack was higher than that of a cathode-facing-cathode two-cell stack during the test procedure. For a three-cell stack, the cell in the middle region presented the highest power output. The open circuit voltage (OCV) and maximum power output of the three-cell stack in a gas mixture of 100 sccm N<sub>2</sub>, 120 sccm CH<sub>4</sub>, and 80 sccm O<sub>2</sub> were 3.0 V and 413 mW, respectively.</p></div>]]></content:encoded><description>Single-chamber solid oxide fuel cell (SC-SOFC) microstacks with V-Shaped congener-electrode-facing configuration were fabricated and operated successfully in a box-like stainless steel chamber. Two gas channels with small gas inlets were used to transport the fuel and oxygen to the anodes and cathodes, respectively. The temperature of an anode-facing-anode two-cell stack was higher than that of a cathode-facing-cathode two-cell stack during the test procedure. For a three-cell stack, the cell in the middle region presented the highest power output. The open circuit voltage (OCV) and maximum power output of the three-cell stack in a gas mixture of 100 sccm N2, 120 sccm CH4, and 80 sccm O2 were 3.0 V and 413 mW, respectively.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100121" xmlns="http://purl.org/rss/1.0/"><title>Enhanced Performance of Solid Oxide Fuel Cell by Manipulating the Orientation of Cylindrical Pores in Anode Substrate</title><link>http://dx.doi.org/10.1002%2Ffuce.201100121</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Enhanced Performance of Solid Oxide Fuel Cell by Manipulating the Orientation of Cylindrical Pores in Anode Substrate</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">W.-P. Pan</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Z. Lü</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">K.-F. Chen</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Y.-H. Zhang</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">B. Wei</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Z.-H. Wang</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">W.-H. Su</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-13T06:34:14.032454-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100121</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/">10.1002/fuce.201100121</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100121</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Effect of the orientation of cylindrical pores within an anode has been studied on the performance of anode-supported solid oxide fuel cell (SOFC). Paper-fibers are used as pore-former and highly oriented cylindrical pores are formed within the anode prepared by uniaxial compaction. A thick anode brick is fabricated followed by cutting in different directions to obtain anode substrates with desirable orientation of pores. When the orientation of cylindrical pores is perpendicular to the anode surface, the gas transport is significantly improved so that the reduction rate of the NiO/YSZ anode is considerably accelerated and the cell concentration polarization is minimized. The corresponding single cell exhibits a maximum power density as high as 1.54 W cm<sup>–2</sup> in hydrogen and 0.90 W cm<sup>–2</sup> in nitrogen diluted methane at 800 °C. The result indicates that the output performance of anode-supported cells could be significantly improved by manipulating the orientation of pores.</p></div>]]></content:encoded><description>Effect of the orientation of cylindrical pores within an anode has been studied on the performance of anode-supported solid oxide fuel cell (SOFC). Paper-fibers are used as pore-former and highly oriented cylindrical pores are formed within the anode prepared by uniaxial compaction. A thick anode brick is fabricated followed by cutting in different directions to obtain anode substrates with desirable orientation of pores. When the orientation of cylindrical pores is perpendicular to the anode surface, the gas transport is significantly improved so that the reduction rate of the NiO/YSZ anode is considerably accelerated and the cell concentration polarization is minimized. The corresponding single cell exhibits a maximum power density as high as 1.54 W cm–2 in hydrogen and 0.90 W cm–2 in nitrogen diluted methane at 800 °C. The result indicates that the output performance of anode-supported cells could be significantly improved by manipulating the orientation of pores.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100126" xmlns="http://purl.org/rss/1.0/"><title>Electrochemical Impedance Analysis of SOFC Cathode Reaction Using Evolutionary Programming</title><link>http://dx.doi.org/10.1002%2Ffuce.201100126</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Electrochemical Impedance Analysis of SOFC Cathode Reaction Using Evolutionary Programming</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Hershkovitz</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Baltianski</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Y. Tsur</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-13T06:34:12.845379-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100126</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/">10.1002/fuce.201100126</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100126</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Investigation of the cathode reaction in solid oxide fuel cells (SOFC) by impedance spectroscopy (IS) measurements using evolutionary-based programming analysis is demonstrated. In contrast to the conventional analysis methods used for impedance spectroscopy measurements, e.g., equivalent circuits, the impedance spectroscopy genetic programming (ISGP) program seeks for a distribution of relaxation times that has the form of a peak or a sum of several peaks, assuming the Debye kernel. Using this method one finds a functional (parametric) form of the distribution of relaxation times. A symmetric cell configuration of Pt|LSCF|GDC|LSCF|Pt was examined using IS measurements combined with <em>I</em>–<em>V</em> measurements. Different samples at different temperatures and different oxygen partial pressures were examined in order to investigate their influence on the oxygen reduction reaction. The resulting IS data was analyzed using the ISGP program and the resulting peaks constructing the distribution of relaxation times were assigned for the different processes that occur at the cathode side. The activation energies as well as the dependence of the processes on the oxygen partial pressure were also evaluated.</p></div>]]></content:encoded><description>Investigation of the cathode reaction in solid oxide fuel cells (SOFC) by impedance spectroscopy (IS) measurements using evolutionary-based programming analysis is demonstrated. In contrast to the conventional analysis methods used for impedance spectroscopy measurements, e.g., equivalent circuits, the impedance spectroscopy genetic programming (ISGP) program seeks for a distribution of relaxation times that has the form of a peak or a sum of several peaks, assuming the Debye kernel. Using this method one finds a functional (parametric) form of the distribution of relaxation times. A symmetric cell configuration of Pt|LSCF|GDC|LSCF|Pt was examined using IS measurements combined with I–V measurements. Different samples at different temperatures and different oxygen partial pressures were examined in order to investigate their influence on the oxygen reduction reaction. The resulting IS data was analyzed using the ISGP program and the resulting peaks constructing the distribution of relaxation times were assigned for the different processes that occur at the cathode side. The activation energies as well as the dependence of the processes on the oxygen partial pressure were also evaluated.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100100" xmlns="http://purl.org/rss/1.0/"><title>Thermal Effect on Water Transport in Proton Exchange Membrane Fuel Cell</title><link>http://dx.doi.org/10.1002%2Ffuce.201100100</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Thermal Effect on Water Transport in Proton Exchange Membrane Fuel Cell</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A. Thomas</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">G. Maranzana</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Didierjean</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. Dillet</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">O. Lottin</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-06T02:11:01.563473-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100100</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/">10.1002/fuce.201100100</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100100</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Adequate water management is critical in proton exchange membrane fuel cells for improving performance and durability. In this paper, we present results of experiments allowing to quantify the effect of a temperature difference between anode and cathode flow field plates on the transport of water. The results confirm the existence of a temperature-gradient driven flux between the anode and cathode compartments. They show the strong interplay between water management and heat management and they confirm that water flows mostly in vapor form through the porous media of the MEA. Apart from the current density and the difference between the temperature of the electrodes and of the flow field plates, the water flux in the direction perpendicular to the membrane is also (weakly) dependent on the humidification of the gases. No significant effect has been measured as a function of the GDL thickness as well as of the presence or absence of a MPL. However, using a MPL improves significantly the performance of the fuel cell.</p></div>]]></content:encoded><description>Adequate water management is critical in proton exchange membrane fuel cells for improving performance and durability. In this paper, we present results of experiments allowing to quantify the effect of a temperature difference between anode and cathode flow field plates on the transport of water. The results confirm the existence of a temperature-gradient driven flux between the anode and cathode compartments. They show the strong interplay between water management and heat management and they confirm that water flows mostly in vapor form through the porous media of the MEA. Apart from the current density and the difference between the temperature of the electrodes and of the flow field plates, the water flux in the direction perpendicular to the membrane is also (weakly) dependent on the humidification of the gases. No significant effect has been measured as a function of the GDL thickness as well as of the presence or absence of a MPL. However, using a MPL improves significantly the performance of the fuel cell.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100070" xmlns="http://purl.org/rss/1.0/"><title>Effect of Ce-Doping on the Electrical and Electrocatalytical Behavior of La/Sr Chromo-Manganite Perovskite as New SOFC Anode</title><link>http://dx.doi.org/10.1002%2Ffuce.201100070</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of Ce-Doping on the Electrical and Electrocatalytical Behavior of La/Sr Chromo-Manganite Perovskite as New SOFC Anode</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">E. Lay</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. Benamira</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">C. Pirovano</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">G. Gauthier</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">L. Dessemond</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-11-22T08:10:28.014059-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100070</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/">10.1002/fuce.201100070</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100070</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The effect of cerium substitution on the electrical and electrochemical characteristics of a new anode material La<sub>0.75</sub>Sr<sub>0.25</sub>Cr<sub>0.5</sub>Mn<sub>0.5</sub>O<sub>3</sub> (LSCM) was examined by synthesizing Ce<sub><em>x</em></sub>La<sub>0.75–</sub><sub><em>x</em></sub>Sr<sub>0.25</sub>Cr<sub>0.5</sub>Mn<sub>0.5</sub>O<sub>3</sub> for <em>x</em> = 0–0.375). From <em>x</em> = 0–0.25, the structure is rhombohedral (S.G. R-3c), and with a higher cerium content (<em>x</em> = 0.375) it becomes cubic (S.G. Pm-3m). These materials are stable in the operating conditions of an SOFC anode. Ce<sub><em>x</em></sub>La<sub>0.75–</sub><sub><em>x</em></sub>Sr<sub>0.25</sub>Cr<sub>0.5</sub>Mn<sub>0.5</sub>O<sub>3</sub> and LSCM materials are p-type semi-conductors. Cerium substitution improves the conductivity in neutral atmosphere from 18.3 to 35.4 S cm<sup>–1</sup> for <em>x</em> = 0 and 0.375, respectively, at 1,173 K. In reducing conditions, the conductivity is not influenced by cerium substitution, and it is about 1 S cm<sup>–1</sup> at 1,173 K. High temperature XRD shows that structure becomes cubic at 1,073 K in operating (reducing) conditions. Cerium substitution positively enhances the electrochemical behavior, as proved by studying the properties of dense cone-shaped electrodes.</p></div>]]></content:encoded><description>The effect of cerium substitution on the electrical and electrochemical characteristics of a new anode material La0.75Sr0.25Cr0.5Mn0.5O3 (LSCM) was examined by synthesizing CexLa0.75–xSr0.25Cr0.5Mn0.5O3 for x = 0–0.375). From x = 0–0.25, the structure is rhombohedral (S.G. R-3c), and with a higher cerium content (x = 0.375) it becomes cubic (S.G. Pm-3m). These materials are stable in the operating conditions of an SOFC anode. CexLa0.75–xSr0.25Cr0.5Mn0.5O3 and LSCM materials are p-type semi-conductors. Cerium substitution improves the conductivity in neutral atmosphere from 18.3 to 35.4 S cm–1 for x = 0 and 0.375, respectively, at 1,173 K. In reducing conditions, the conductivity is not influenced by cerium substitution, and it is about 1 S cm–1 at 1,173 K. High temperature XRD shows that structure becomes cubic at 1,073 K in operating (reducing) conditions. Cerium substitution positively enhances the electrochemical behavior, as proved by studying the properties of dense cone-shaped electrodes.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100051" xmlns="http://purl.org/rss/1.0/"><title>Synthesis and Characterization of Polymer Blends of Sulfonated Polyethersulfone and Sulfonated Polyethersulfone Octylsulfonamide for PEMFC Applications</title><link>http://dx.doi.org/10.1002%2Ffuce.201100051</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Synthesis and Characterization of Polymer Blends of Sulfonated Polyethersulfone and Sulfonated Polyethersulfone Octylsulfonamide for PEMFC Applications</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">W. Mabrouk</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">L. Ogier</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Vidal</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">C. Sollogoub</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">F. Matoussi</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. Dachraoui</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. F. Fauvarque</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-11-22T08:10:21.670733-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100051</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/">10.1002/fuce.201100051</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100051</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Our goal in the present work was to synthesize a new proton exchange membrane that could be used in proton exchange membrane fuel cell (PEMFC), based on a blend of sulfonated polyethersulfone (S-PES) and sulfonated polyethersulfone octylsulfonamide (S-PESOS). Five blends, using S-PESOS with different grafting ratios of sulfonamide groups, have been elaborated, characterized, and tested in a PEMFC. The similar chemical structure between these two polymers favored their compatibility. The synthesized membranes showed a high water swelling capacity and an ionic conductivity equivalent to that of Nafion® (0.1 S cm<sup>–1</sup>) in the same conditions.</p></div>]]></content:encoded><description>Our goal in the present work was to synthesize a new proton exchange membrane that could be used in proton exchange membrane fuel cell (PEMFC), based on a blend of sulfonated polyethersulfone (S-PES) and sulfonated polyethersulfone octylsulfonamide (S-PESOS). Five blends, using S-PESOS with different grafting ratios of sulfonamide groups, have been elaborated, characterized, and tested in a PEMFC. The similar chemical structure between these two polymers favored their compatibility. The synthesized membranes showed a high water swelling capacity and an ionic conductivity equivalent to that of Nafion® (0.1 S cm–1) in the same conditions.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100098" xmlns="http://purl.org/rss/1.0/"><title>A H2/O2 Fuel Cell for In situ μ-Raman Measurements. In-depth Characterization of an Ionic Liquid Filled Nafion Membrane</title><link>http://dx.doi.org/10.1002%2Ffuce.201100098</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A H2/O2 Fuel Cell for In situ μ-Raman Measurements. In-depth Characterization of an Ionic Liquid Filled Nafion Membrane</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A. Martinelli</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">C. Iojoiu</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">N. Sergent</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-11-11T04:50:50.807344-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100098</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/">10.1002/fuce.201100098</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100098</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>We report the design of a H<sub>2</sub>/O<sub>2</sub> (fuel) cell for <em>in situ</em> μ-Raman spectroscopic measurements. The horizontal orientation of the cell is conceived to allow the penetration of the laser beam along the z-axis from one electrode to the other. We show that during in-depth analyses the Raman signal is not significantly lost and the axial resolution is sufficiently good to allow quantitative and qualitative spectral interpretation. We report “proof of principle” tests performed on Nafion membranes swelled with protic ionic liquids to demonstrate the validity of the design and the potentiality of the method. Our results confirm that this experimental setup can efficiently be used to follow structural changes and concentration gradients in the electrolyte of a fuel cell <em>operando</em>. In particular, we have been able to resolve both in time and in space the hydration state of the membrane as well as spatial variations for the <span class="math"><img alt="equation image" src="http://onlinelibrary.wiley.com/store/10.1002/fuce.201100098/asset/equation/tex2gif-ueqn-1.gif?v=1&amp;t=gymvleqx&amp;s=9571151dbf4235cde16d380e9d269f92b6146a46" class="inlineGraphic"/></span> coordination shell during a compositional transient state.</p></div>]]></content:encoded><description>We report the design of a H2/O2 (fuel) cell for in situ μ-Raman spectroscopic measurements. The horizontal orientation of the cell is conceived to allow the penetration of the laser beam along the z-axis from one electrode to the other. We show that during in-depth analyses the Raman signal is not significantly lost and the axial resolution is sufficiently good to allow quantitative and qualitative spectral interpretation. We report “proof of principle” tests performed on Nafion membranes swelled with protic ionic liquids to demonstrate the validity of the design and the potentiality of the method. Our results confirm that this experimental setup can efficiently be used to follow structural changes and concentration gradients in the electrolyte of a fuel cell operando. In particular, we have been able to resolve both in time and in space the hydration state of the membrane as well as spatial variations for the $ {\rm SO}_3^- $ coordination shell during a compositional transient state.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100080" xmlns="http://purl.org/rss/1.0/"><title>Characterization of Uncoated Stainless Steel as Proton Exchange Membrane Fuel Cell Bipolar Plates material</title><link>http://dx.doi.org/10.1002%2Ffuce.201100080</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Characterization of Uncoated Stainless Steel as Proton Exchange Membrane Fuel Cell Bipolar Plates material</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">N. Caqué</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. Paris</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. Chatenet</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">E. Rossinot</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">R. Bousquet</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">E. Claude</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-10-05T10:31:49.429926-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100080</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/">10.1002/fuce.201100080</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100080</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Thanks to their high conductivity, important gas tightness, good corrosion resistance, and low-cost manufacturing pathways, stainless steels are considered as good candidates for proton exchange membrane fuel cell (PEMFC) bipolar plates materials. In this study, a proprietary alloy was identified as very promising: its initial electrical contact resistance (ECR) with the gas diffusion layer was low, while its corrosion resistance in simulated PEMFC environment was sufficient. Furthermore, the ECR did not increase dramatically during long-term potentiostatic and potentiodynamic polarizations in simulated PEMFC cathode and anode environments. Finally, the stainless steel was successfully tested for 3,000 h in a commercial system using a 16-cell stack, without detrimental cell voltage losses.</p></div>]]></content:encoded><description>Thanks to their high conductivity, important gas tightness, good corrosion resistance, and low-cost manufacturing pathways, stainless steels are considered as good candidates for proton exchange membrane fuel cell (PEMFC) bipolar plates materials. In this study, a proprietary alloy was identified as very promising: its initial electrical contact resistance (ECR) with the gas diffusion layer was low, while its corrosion resistance in simulated PEMFC environment was sufficient. Furthermore, the ECR did not increase dramatically during long-term potentiostatic and potentiodynamic polarizations in simulated PEMFC cathode and anode environments. Finally, the stainless steel was successfully tested for 3,000 h in a commercial system using a 16-cell stack, without detrimental cell voltage losses.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100079" xmlns="http://purl.org/rss/1.0/"><title>Catalytic Steam Methane Reforming Over Ir/Ce0.9Gd0.1O2–x: Resistance to Coke Formation and Sulfur Poisoning</title><link>http://dx.doi.org/10.1002%2Ffuce.201100079</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Catalytic Steam Methane Reforming Over Ir/Ce0.9Gd0.1O2–x: Resistance to Coke Formation and Sulfur Poisoning</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">G. Postole</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">K. Girona</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. Toyir</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A. Kaddouri</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">P. Gélin</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-08-03T08:20:28.776362-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100079</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/">10.1002/fuce.201100079</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100079</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>This work investigates the catalytic properties of Ir/Ce<sub>0.9</sub>Gd<sub>0.1</sub>O<sub>2–</sub><sub><em>x</em></sub> (Ir/CGO) catalyst and CGO support in steam reforming of methane in the absence or presence of H<sub>2</sub>S (50 ppm) for further application in a solid oxide fuel cell (SOFC) working under methane at intermediate temperatures and integrating a gradual internal reforming concept. The catalytic activity was measured at 750 °C by using a 50 mol.% CH<sub>4</sub>/5 mol.% H<sub>2</sub>O/45 mol.% N<sub>2</sub> mixture and a 10 mol.% CH<sub>4</sub>/90 mol.% N<sub>2</sub> mixture. The addition of Ir to CGO improves the catalytic activity in hydrogen production by two orders of magnitude with respect to that of CGO alone. Temperature programmed oxidation experiments were performed after reaction in both types of mixtures to study the eventual formation of carbon deposits. Over Ir/CGO, carbon formed in little amounts (even in the absence of H<sub>2</sub>O in the feed), being highly reactive toward O<sub>2</sub>. Upon H<sub>2</sub>S addition, the CGO support exhibited surprisingly an improved catalytic activity on the contrary to Ir/CGO which partly deactivated. Upon suppression of H<sub>2</sub>S in the feed the initial catalytic activity was fully restored for both catalysts. The catalytic behavior of CGO in the presence of H<sub>2</sub>S was discussed, based upon temperature programmed reaction of CH<sub>4</sub>.</p></div>]]></content:encoded><description>This work investigates the catalytic properties of Ir/Ce0.9Gd0.1O2–x (Ir/CGO) catalyst and CGO support in steam reforming of methane in the absence or presence of H2S (50 ppm) for further application in a solid oxide fuel cell (SOFC) working under methane at intermediate temperatures and integrating a gradual internal reforming concept. The catalytic activity was measured at 750 °C by using a 50 mol.% CH4/5 mol.% H2O/45 mol.% N2 mixture and a 10 mol.% CH4/90 mol.% N2 mixture. The addition of Ir to CGO improves the catalytic activity in hydrogen production by two orders of magnitude with respect to that of CGO alone. Temperature programmed oxidation experiments were performed after reaction in both types of mixtures to study the eventual formation of carbon deposits. Over Ir/CGO, carbon formed in little amounts (even in the absence of H2O in the feed), being highly reactive toward O2. Upon H2S addition, the CGO support exhibited surprisingly an improved catalytic activity on the contrary to Ir/CGO which partly deactivated. Upon suppression of H2S in the feed the initial catalytic activity was fully restored for both catalysts. The catalytic behavior of CGO in the presence of H2S was discussed, based upon temperature programmed reaction of CH4.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100033" xmlns="http://purl.org/rss/1.0/"><title>Evolution of Water Distribution in PEMFC during On/Off Cycling</title><link>http://dx.doi.org/10.1002%2Ffuce.201100033</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Evolution of Water Distribution in PEMFC during On/Off Cycling</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A. Morin</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">F. Xu</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">G. Gebel</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">O. Diat</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-08-03T08:20:23.23154-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100033</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/">10.1002/fuce.201100033</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100033</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The evolution of membrane water concentration profile has been studied by small angle neutron scattering during on/off cycling PEMFC operation with fully humidified air in co-flow configuration. The water concentration profiles during on/off cycling evolve in opposite ways close to the gas inlet and outlet. Whereas the global membrane water content increases at the gas inlet as the fuel cell delivers current, the membranes are dried out at the gas outlet. The balance between the diffusion of water from cathode to anode and the electroosmostic drag from anode to cathode gives a net flow which is different close to the gas inlet and gas outlet. The equilibrium is reached in less than 15 min and it is faster when the fuel cell is switched on that is to say when a proton flows is imposed. Moreoever, the time to equilibrium decreases as the membrane content is increased.</p></div>]]></content:encoded><description>The evolution of membrane water concentration profile has been studied by small angle neutron scattering during on/off cycling PEMFC operation with fully humidified air in co-flow configuration. The water concentration profiles during on/off cycling evolve in opposite ways close to the gas inlet and outlet. Whereas the global membrane water content increases at the gas inlet as the fuel cell delivers current, the membranes are dried out at the gas outlet. The balance between the diffusion of water from cathode to anode and the electroosmostic drag from anode to cathode gives a net flow which is different close to the gas inlet and gas outlet. The equilibrium is reached in less than 15 min and it is faster when the fuel cell is switched on that is to say when a proton flows is imposed. Moreoever, the time to equilibrium decreases as the membrane content is increased.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100053" xmlns="http://purl.org/rss/1.0/"><title>Influence of Compressive Stress on the Water Content of Perfluorosulphonated Membranes: A μ-Raman Study</title><link>http://dx.doi.org/10.1002%2Ffuce.201100053</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Influence of Compressive Stress on the Water Content of Perfluorosulphonated Membranes: A μ-Raman Study</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A. K. Sutor</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">P. Huguet</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A. Morin</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">G. Gebel</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">T. S. Le</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Deabate</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-07-15T03:10:22.96914-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100053</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/">10.1002/fuce.201100053</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100053</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The effect of compressive stress on the local water content of Nafion NRE 212 and Aquivion E79 membranes is studied by confocal μ-Raman spectroscopy using a specific tightening device. This device aims to mimic the geometry of the bipolar plate flow field of actual fuel cells, i.e. the sequence of channels and ribs. The membrane water content decreases with increasing stress, under the ribs as well as in the channel. The higher the initial water content, the larger the water content decreases with mechanical stress. The extent of water loss depends on the position of the membrane in the device, the applied stress and the hydration history of the membrane.</p></div>]]></content:encoded><description>The effect of compressive stress on the local water content of Nafion NRE 212 and Aquivion E79 membranes is studied by confocal μ-Raman spectroscopy using a specific tightening device. This device aims to mimic the geometry of the bipolar plate flow field of actual fuel cells, i.e. the sequence of channels and ribs. The membrane water content decreases with increasing stress, under the ribs as well as in the channel. The higher the initial water content, the larger the water content decreases with mechanical stress. The extent of water loss depends on the position of the membrane in the device, the applied stress and the hydration history of the membrane.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100042" xmlns="http://purl.org/rss/1.0/"><title>Alumina–Carbon Nanofibers Nanocomposites Obtained by Spark Plasma Sintering for Proton Exchange Membrane Fuel Cell Bipolar Plates</title><link>http://dx.doi.org/10.1002%2Ffuce.201100042</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Alumina–Carbon Nanofibers Nanocomposites Obtained by Spark Plasma Sintering for Proton Exchange Membrane Fuel Cell Bipolar Plates</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A. Borrell</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">R. Torrecillas</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">V. G. Rocha</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A. Fernández</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-06-10T06:20:19.305349-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100042</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/">10.1002/fuce.201100042</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100042</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</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[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>There is an increasing demand of multifunctional materials for a wide variety of technological developments. Bipolar plates for proton exchange membrane fuel cells are an example of complex functionality components that must show among other properties high mechanical strength, electrical, and thermal conductivity. The present research explored the possibility of using alumina–carbon nanofibers (CNFs) nanocomposites for this purpose. In this study, it was studied for the first time the whole range of powder compositions in this system. Homogeneous powders mixtures were prepared and subsequently sintered by spark plasma sintering. The materials obtained were thoroughly characterized and compared in terms of properties required to be used as bipolar plates. The control on material microstructure and composition allows designing materials where mechanical or electrical performances are enhanced. A 50/50 vol.% alumina–CNFs composite appears to be a very promising material for this kind of application.</p></div>]]></content:encoded><description>There is an increasing demand of multifunctional materials for a wide variety of technological developments. Bipolar plates for proton exchange membrane fuel cells are an example of complex functionality components that must show among other properties high mechanical strength, electrical, and thermal conductivity. The present research explored the possibility of using alumina–carbon nanofibers (CNFs) nanocomposites for this purpose. In this study, it was studied for the first time the whole range of powder compositions in this system. Homogeneous powders mixtures were prepared and subsequently sintered by spark plasma sintering. The materials obtained were thoroughly characterized and compared in terms of properties required to be used as bipolar plates. The control on material microstructure and composition allows designing materials where mechanical or electrical performances are enhanced. A 50/50 vol.% alumina–CNFs composite appears to be a very promising material for this kind of application.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201190020" xmlns="http://purl.org/rss/1.0/"><title>Cover Fuel Cells 6/2011</title><link>http://dx.doi.org/10.1002%2Ffuce.201190020</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Cover Fuel Cells 6/2011</dc:title><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201190020</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/">10.1002/fuce.201190020</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201190020</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Cover Picture</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[]]></content:encoded><description/></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201190021" xmlns="http://purl.org/rss/1.0/"><title>Editorial Board Fuel Cells 6/2011</title><link>http://dx.doi.org/10.1002%2Ffuce.201190021</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Editorial Board Fuel Cells 6/2011</dc:title><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201190021</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/">10.1002/fuce.201190021</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201190021</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Editorial Board</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[]]></content:encoded><description/></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201190018" xmlns="http://purl.org/rss/1.0/"><title>Contents: Fuel Cells 6/2011</title><link>http://dx.doi.org/10.1002%2Ffuce.201190018</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Contents: Fuel Cells 6/2011</dc:title><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201190018</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/">10.1002/fuce.201190018</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201190018</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Contents</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">711</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">713</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[]]></content:encoded><description/></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201190019" xmlns="http://purl.org/rss/1.0/"><title>International Conference on Progress in MEA Materials for Medium and High Temperature Polymer Electrolyte Fuel Cells</title><link>http://dx.doi.org/10.1002%2Ffuce.201190019</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">International Conference on Progress in MEA Materials for Medium and High Temperature Polymer Electrolyte Fuel Cells</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">D. Jones</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201190019</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/">10.1002/fuce.201190019</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201190019</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Editorial</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">714</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">714</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[]]></content:encoded><description/></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201000180" xmlns="http://purl.org/rss/1.0/"><title>Graphitised Carbon Nanofibres as Catalyst Support for PEMFC</title><link>http://dx.doi.org/10.1002%2Ffuce.201000180</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Graphitised Carbon Nanofibres as Catalyst Support for PEMFC</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">E. Yli-Rantala</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A. Pasanen</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">P. Kauranen</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">V. Ruiz</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. Borghei</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">E. Kauppinen</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A. Oyarce</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">G. Lindbergh</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">C. Lagergren</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. Darab</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Sunde</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. Thomassen</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Ma-Andersen</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">E. Skou.</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201000180</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/">10.1002/fuce.201000180</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201000180</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">715</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">725</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Graphitised carbon nanofibres (G-CNFs) show superior thermal stability and corrosion resistance in PEM fuel cell environment over traditional carbon black (CB) and carbon nanotube catalyst supports. However, G-CNFs have an inert surface with only very limited amount of surface defects for the anchorage of Pt catalyst nanoparticles. Modification of the fibre surface is therefore needed. In this study Pt nanoparticles have been deposited onto as-received and surface-modified G-CNFs. The surface modifications of the fibres comprise acid treatment and nitrogen doping by pyrolysis of a polyaniline (PANI) precursor. The modified surfaces were studied by FTIR and XPS and the electrochemical characterization, including long-term Pt stability tests, was performed using a low-temperature PEMFC single cell. The performance and stability of the G-CNF supported catalysts were compared with a CB supported catalyst and the effects of the different surface treatments were discussed. On the basis of these results, new membrane electrode assemblies (MEAs) were manufactured and tested also for carbon corrosion by <em>in situ</em> FTIR analysis of the cathode exhaust gases. It was observed that the G-CNFs showed 5 times lower carbon corrosion compared to CB based catalyst when potential reached 1.5 V <em>versus</em> RHE in simulated start/stop cycling.</p></div>]]></content:encoded><description>Graphitised carbon nanofibres (G-CNFs) show superior thermal stability and corrosion resistance in PEM fuel cell environment over traditional carbon black (CB) and carbon nanotube catalyst supports. However, G-CNFs have an inert surface with only very limited amount of surface defects for the anchorage of Pt catalyst nanoparticles. Modification of the fibre surface is therefore needed. In this study Pt nanoparticles have been deposited onto as-received and surface-modified G-CNFs. The surface modifications of the fibres comprise acid treatment and nitrogen doping by pyrolysis of a polyaniline (PANI) precursor. The modified surfaces were studied by FTIR and XPS and the electrochemical characterization, including long-term Pt stability tests, was performed using a low-temperature PEMFC single cell. The performance and stability of the G-CNF supported catalysts were compared with a CB supported catalyst and the effects of the different surface treatments were discussed. On the basis of these results, new membrane electrode assemblies (MEAs) were manufactured and tested also for carbon corrosion by in situ FTIR analysis of the cathode exhaust gases. It was observed that the G-CNFs showed 5 times lower carbon corrosion compared to CB based catalyst when potential reached 1.5 V versus RHE in simulated start/stop cycling.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201000182" xmlns="http://purl.org/rss/1.0/"><title>Carbon Aerogels as Catalyst Supports and First Insights on Their Durability in Proton Exchange Membrane Fuel Cells</title><link>http://dx.doi.org/10.1002%2Ffuce.201000182</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Carbon Aerogels as Catalyst Supports and First Insights on Their Durability in Proton Exchange Membrane Fuel Cells</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. Ouattara-Brigaudet</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">C. Beauger</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Berthon-Fabry</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">P. Achard</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201000182</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/">10.1002/fuce.201000182</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201000182</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">726</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">734</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>To enable a large penetration of proton exchange membrane fuel cells (PEMFC) on the market, the durability of these systems must be improved. This work aims at evaluating the durability of carbon aerogels used as cathode catalyst support and at comparing it with the durability of a commercial electrocatalyst Tanaka Kikinzoku Group (TKK). To do so, platinum was deposited on carbon aerogel. Resulting electrocatalysts were then used to prepare 50 cm<sup>2</sup> membrane electrode assemblies (MEA). MEAs were then submitted to an ageing protocol consisting in operating the cell under H<sub>2</sub>/N<sub>2</sub> and in maintaining the cell potential at 1.2 V during cycles of 7 h. MEA performance was then evaluated every 7 h before the following cycle. We showed that, in our testing conditions, neither carbon aerogel nor the commercial electrocatalyst can fulfil DOE objectives in terms of durability. The lower carbon aerogel corrosion resistance as compared to that one of the commercial electrocatalyst can be explained by their low degree of graphitisation. Carbon aerogels durability could be increased thanks to a pyrolysis at higher temperatures.</p></div>]]></content:encoded><description>To enable a large penetration of proton exchange membrane fuel cells (PEMFC) on the market, the durability of these systems must be improved. This work aims at evaluating the durability of carbon aerogels used as cathode catalyst support and at comparing it with the durability of a commercial electrocatalyst Tanaka Kikinzoku Group (TKK). To do so, platinum was deposited on carbon aerogel. Resulting electrocatalysts were then used to prepare 50 cm2 membrane electrode assemblies (MEA). MEAs were then submitted to an ageing protocol consisting in operating the cell under H2/N2 and in maintaining the cell potential at 1.2 V during cycles of 7 h. MEA performance was then evaluated every 7 h before the following cycle. We showed that, in our testing conditions, neither carbon aerogel nor the commercial electrocatalyst can fulfil DOE objectives in terms of durability. The lower carbon aerogel corrosion resistance as compared to that one of the commercial electrocatalyst can be explained by their low degree of graphitisation. Carbon aerogels durability could be increased thanks to a pyrolysis at higher temperatures.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201000187" xmlns="http://purl.org/rss/1.0/"><title>High-Temperature Electrochemical Characterization of Ru Core Pt Shell Fuel Cell Catalyst</title><link>http://dx.doi.org/10.1002%2Ffuce.201000187</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">High-Temperature Electrochemical Characterization of Ru Core Pt Shell Fuel Cell Catalyst</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">D. Bokach</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. L. G. de la Fuente</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. Tsypkin</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">P. Ochal</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">I. C. Endsjø</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">R. Tunold</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Sunde</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">F. Seland</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201000187</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/">10.1002/fuce.201000187</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201000187</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">735</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">744</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The electrooxidation of methanol was studied at elevated temperature and pressure by cyclic voltammetry and constant potential experiments at real fuel cell electrocatalysts. Ruthenium core and platinum shell nanoparticles were synthesized by a sequential polyol route, and characterized electrochemically by CO stripping at room temperature to quickly confirm the structure of the synthesized core–shell structure as compared to pure commercial Pt/C and Pt–Ru/C alloy catalysts. A significant promotional effect of Pt decorated Ru cores in the methanol oxidation was found at elevated temperatures and rather high-electrode potentials. A negative potential shift of the methanol oxidation peak is observed for the Ru@Pt/C core–shell catalyst at moderate temperatures, while a significant shift to positive potentials of the methanol oxidation peak occurs for Pt/C catalysts. The onset potential for methanol oxidation is lowered some 200 mV from room temperature and up to 120 °C for all electrocatalysts, indicating that it is the thermal activity of water adsorption that dictates the onset potential. Direct methanol fuel cell experiments showed only small performance differences between Ru@Pt/C and Pt/C anode electrocatalysts, suggesting the necessity of render possible the formation of surface oxygen species at lower electrode potentials.</p></div>]]></content:encoded><description>The electrooxidation of methanol was studied at elevated temperature and pressure by cyclic voltammetry and constant potential experiments at real fuel cell electrocatalysts. Ruthenium core and platinum shell nanoparticles were synthesized by a sequential polyol route, and characterized electrochemically by CO stripping at room temperature to quickly confirm the structure of the synthesized core–shell structure as compared to pure commercial Pt/C and Pt–Ru/C alloy catalysts. A significant promotional effect of Pt decorated Ru cores in the methanol oxidation was found at elevated temperatures and rather high-electrode potentials. A negative potential shift of the methanol oxidation peak is observed for the Ru@Pt/C core–shell catalyst at moderate temperatures, while a significant shift to positive potentials of the methanol oxidation peak occurs for Pt/C catalysts. The onset potential for methanol oxidation is lowered some 200 mV from room temperature and up to 120 °C for all electrocatalysts, indicating that it is the thermal activity of water adsorption that dictates the onset potential. Direct methanol fuel cell experiments showed only small performance differences between Ru@Pt/C and Pt/C anode electrocatalysts, suggesting the necessity of render possible the formation of surface oxygen species at lower electrode potentials.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201000146" xmlns="http://purl.org/rss/1.0/"><title>Oxidative Degradation of Polybenzimidazole Membranes as Electrolytes for High Temperature Proton Exchange Membrane Fuel Cells</title><link>http://dx.doi.org/10.1002%2Ffuce.201000146</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Oxidative Degradation of Polybenzimidazole Membranes as Electrolytes for High Temperature Proton Exchange Membrane Fuel Cells</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. H. Liao</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Q. F. Li</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">H. C. Rudbeck</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. O. Jensen</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A. Chromik</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">N. J. Bjerrum</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. Kerres</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">W. Xing</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201000146</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/">10.1002/fuce.201000146</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201000146</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">745</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">755</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Polybenzimidazole membranes imbibed with acid are emerging as a suitable electrolyte material for high-temperature polymer electrolyte fuel cells. The oxidative stability of polybenzimidazole has been identified as an important issue for the long-term durability of such cells. In this paper the oxidative degradation of the polymer membrane was studied under the Fenton test conditions by the weight loss, intrinsic viscosity, size exclusion chromatography, scanning electron microscopy and Fourier transform infrared spectroscopy. During the Fenton test, significant weight losses depending on the initial molecular weight of the polymer were observed. At the same time, viscosity and SEC measurements revealed a steady decrease in molecular weight. The degradation of acid doped PBI membranes under Fenton test conditions is proposed to start by the attack of hydroxyl radicals at the carbon atom linking imidazole ring and benzenoid ring, which may eventually lead to the imidazole ring opening and formation of small molecules and terminal groups for further oxidation by an endpoint oxidation.</p></div>]]></content:encoded><description>Polybenzimidazole membranes imbibed with acid are emerging as a suitable electrolyte material for high-temperature polymer electrolyte fuel cells. The oxidative stability of polybenzimidazole has been identified as an important issue for the long-term durability of such cells. In this paper the oxidative degradation of the polymer membrane was studied under the Fenton test conditions by the weight loss, intrinsic viscosity, size exclusion chromatography, scanning electron microscopy and Fourier transform infrared spectroscopy. During the Fenton test, significant weight losses depending on the initial molecular weight of the polymer were observed. At the same time, viscosity and SEC measurements revealed a steady decrease in molecular weight. The degradation of acid doped PBI membranes under Fenton test conditions is proposed to start by the attack of hydroxyl radicals at the carbon atom linking imidazole ring and benzenoid ring, which may eventually lead to the imidazole ring opening and formation of small molecules and terminal groups for further oxidation by an endpoint oxidation.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201000148" xmlns="http://purl.org/rss/1.0/"><title>Thermal Behaviours and Single Cell Performance of PBI-OO/PFSA Blend Membranes Composited with Lewis Acid Nanoparticles for Intermediate Temperature DMFC Application</title><link>http://dx.doi.org/10.1002%2Ffuce.201000148</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Thermal Behaviours and Single Cell Performance of PBI-OO/PFSA Blend Membranes Composited with Lewis Acid Nanoparticles for Intermediate Temperature DMFC Application</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. Hu</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. Luo</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">P. Wagner</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">C. Agert</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">O. Conrad</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201000148</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/">10.1002/fuce.201000148</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201000148</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">756</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">763</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Building on the improved proton conductivity at intermediate temperatures under anhydrous conditions using a ‘proton donor–proton acceptor' concept demonstrated for the first time in the composite membrane made of inorganic lewis acid (boron-based electron-deficient nanoparticles) and a poly-[(1-(4,4′-diphenylether)-5-oxybenzimidazole)-benzimidazole] (PBI-OO)/perfluorosulfonic acid (PFSA) blend, we report here the thermal behaviours and direct methanol fuel cell (DMFC) single cell performance of these membranes at intermediate temperatures (90–120 °C). It is found that the PFSA/PBI-OO blends and PFSA/PBI-OO/nano-BN composites show decreased thermal stability compared to pristine PFSA. We attribute this to a proton transfer reaction between the sulfonic acid and imidazole moieties of the constituent polymers inducing a decreased stability of the resulting sulfonate group. When operated with dry oxygen and methanol/water vapour, the single cell performance of PFSA/PBI-OO blends is slightly improved compared to that of pristine PFSA. The PFSA/PBI-OO/nano-BN composite membranes exhibit much better single cell performance at intermediate temperatures, which could be mainly attributed to its higher anhydrous proton conductivity.</p></div>]]></content:encoded><description>Building on the improved proton conductivity at intermediate temperatures under anhydrous conditions using a ‘proton donor–proton acceptor' concept demonstrated for the first time in the composite membrane made of inorganic lewis acid (boron-based electron-deficient nanoparticles) and a poly-[(1-(4,4′-diphenylether)-5-oxybenzimidazole)-benzimidazole] (PBI-OO)/perfluorosulfonic acid (PFSA) blend, we report here the thermal behaviours and direct methanol fuel cell (DMFC) single cell performance of these membranes at intermediate temperatures (90–120 °C). It is found that the PFSA/PBI-OO blends and PFSA/PBI-OO/nano-BN composites show decreased thermal stability compared to pristine PFSA. We attribute this to a proton transfer reaction between the sulfonic acid and imidazole moieties of the constituent polymers inducing a decreased stability of the resulting sulfonate group. When operated with dry oxygen and methanol/water vapour, the single cell performance of PFSA/PBI-OO blends is slightly improved compared to that of pristine PFSA. The PFSA/PBI-OO/nano-BN composite membranes exhibit much better single cell performance at intermediate temperatures, which could be mainly attributed to its higher anhydrous proton conductivity.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201000179" xmlns="http://purl.org/rss/1.0/"><title>Application of CFD Techniques in the Modelling and Simulation of PBI PEMFC</title><link>http://dx.doi.org/10.1002%2Ffuce.201000179</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Application of CFD Techniques in the Modelling and Simulation of PBI PEMFC</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">G. Doubek</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">E. Robalinho</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">E. F. Cunha</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">E. Cekinski</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. Linardi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201000179</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/">10.1002/fuce.201000179</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201000179</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">764</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">774</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>In the present work two 3-D models, for the catalytic layer, were employed in order to simulate the responses of a PBI high temperature polymeric membrane fuel cell. The simulations made use of an agglomerate model and a pseudo-homogenous model, both implemented taking into account the temperature influence over their parameters. The overall simulation was performed also as two models, linked by the variable pressure, one for the whole graphite plate simulating the distribution channels, and the other dealing with the MEA and thereof the catalytic layer. A discussion over the two models was done and the experimental results demonstrated that the pseudo-homogeneous obtained the better fits.</p></div>]]></content:encoded><description>In the present work two 3-D models, for the catalytic layer, were employed in order to simulate the responses of a PBI high temperature polymeric membrane fuel cell. The simulations made use of an agglomerate model and a pseudo-homogenous model, both implemented taking into account the temperature influence over their parameters. The overall simulation was performed also as two models, linked by the variable pressure, one for the whole graphite plate simulating the distribution channels, and the other dealing with the MEA and thereof the catalytic layer. A discussion over the two models was done and the experimental results demonstrated that the pseudo-homogeneous obtained the better fits.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201000189" xmlns="http://purl.org/rss/1.0/"><title>Progress in PEMFC MEA Component R&amp;D at the DOE Fuel Cell Technologies Program</title><link>http://dx.doi.org/10.1002%2Ffuce.201000189</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Progress in PEMFC MEA Component R&amp;D at the DOE Fuel Cell Technologies Program</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. S. Spendelow</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">D. C. Papageorgopoulos</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201000189</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/">10.1002/fuce.201000189</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201000189</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">775</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">786</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The U.S. Department of Energy Fuel Cell Technologies Program supports research and development (R&amp;D) of fuel cells and fuel cell systems for stationary, portable and transportation applications. The Program maintains a diverse portfolio of R&amp;D projects aimed at reducing cost and improving durability of fuel cell systems, with an overarching goal of enabling fuel cell technology to compete with alternative technologies in the marketplace. This paper describes the Program's recent activities and progress in development of catalysts, membranes and membrane electrode assemblies for polymer electrolyte membrane fuel cells.</p></div>]]></content:encoded><description>The U.S. Department of Energy Fuel Cell Technologies Program supports research and development (R&amp;D) of fuel cells and fuel cell systems for stationary, portable and transportation applications. The Program maintains a diverse portfolio of R&amp;D projects aimed at reducing cost and improving durability of fuel cell systems, with an overarching goal of enabling fuel cell technology to compete with alternative technologies in the marketplace. This paper describes the Program's recent activities and progress in development of catalysts, membranes and membrane electrode assemblies for polymer electrolyte membrane fuel cells.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201000167" xmlns="http://purl.org/rss/1.0/"><title>Highly Sulphonated Multiblock-co-polymers for Direct Methanol Fuel Cells</title><link>http://dx.doi.org/10.1002%2Ffuce.201000167</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Highly Sulphonated Multiblock-co-polymers for Direct Methanol Fuel Cells</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">K. Krajinovic</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">T. Kaz</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">T. Haering</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">V. Gogel</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. Kerres</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201000167</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/">10.1002/fuce.201000167</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201000167</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">787</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">800</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Multiblock-<em>co</em>-polymers with different ion exchange capacities were synthesised by nucleophilic aromatic step-growth polycondensation of hydrophilic and hydrophobic oligomers. The main focus of this work was to investigate the dependence of oligomer reactivity on molecular weight and how the reaction conditions need to be changed to obtain high-molecular multiblock-<em>co</em>-polymers, consisting of long block segments. Multiblock-<em>co</em>-polymers composed of short oligomers could be synthesised under mild reaction conditions. The coupling of longer oligomers required more basic reaction conditions, because the reactive functional end-groups were shielded by the long oligomeric main chain. The membranes were investigated further in terms of their properties relevant for use as polymer electrolyte membrane in direct methanol fuel cells (DMFCs). The mechanical stability of the acidic polymers was improved through ionical crosslinking with basic polybenzimidazole. A series of membranes was tested in a self- and in an air-breathing DMFC.</p></div>]]></content:encoded><description>Multiblock-co-polymers with different ion exchange capacities were synthesised by nucleophilic aromatic step-growth polycondensation of hydrophilic and hydrophobic oligomers. The main focus of this work was to investigate the dependence of oligomer reactivity on molecular weight and how the reaction conditions need to be changed to obtain high-molecular multiblock-co-polymers, consisting of long block segments. Multiblock-co-polymers composed of short oligomers could be synthesised under mild reaction conditions. The coupling of longer oligomers required more basic reaction conditions, because the reactive functional end-groups were shielded by the long oligomeric main chain. The membranes were investigated further in terms of their properties relevant for use as polymer electrolyte membrane in direct methanol fuel cells (DMFCs). The mechanical stability of the acidic polymers was improved through ionical crosslinking with basic polybenzimidazole. A series of membranes was tested in a self- and in an air-breathing DMFC.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201000178" xmlns="http://purl.org/rss/1.0/"><title>Transport Properties of Zeolite Na-X–Nafion Membranes: Effect of Zeolite Loadings and Particle Size</title><link>http://dx.doi.org/10.1002%2Ffuce.201000178</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Transport Properties of Zeolite Na-X–Nafion Membranes: Effect of Zeolite Loadings and Particle Size</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. Lavorgna</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">L. Sansone</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">G. Scherillo</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">R. Gu</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A. P. Baker</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201000178</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/">10.1002/fuce.201000178</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201000178</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">801</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">813</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Na-X zeolites particles, synthesized in two size ranges, namely 200–300 nm and 30–100 nm, were used to prepare Nafion/Na-X zeolite composite membranes by recast method. The physical, chemical, and morphological properties of the zeolite powders and composite membranes were examined by XRD, N<sub>2</sub> adsorption isotherms, FTIR, SEM, and SAXS analysis. Furthermore, the effect of zeolite particles size and loadings (i.e., 5 and 10% w/w) on the water, methanol, and proton transport properties was investigated.</p></div><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>It has been found that the size of the Na-X zeolite particles plays a key role in the proton and methanol transport behavior since it rules the zeolite hydrophilic behavior, the morphology of polymer–filler interphase, and also the nature of water established in the composite membrane.</p></div><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The results show that the membranes loaded with a 5% w/w of submicron-sized Na-X zeolite exhibit a proton conductivity and selectivity significantly higher than Nafion. In particular the proton conductivity at 120 °C is around eight times and the selectivity at 25 °C is around 40% higher than those exhibited by recast Nafion.</p></div>]]></content:encoded><description>Na-X zeolites particles, synthesized in two size ranges, namely 200–300 nm and 30–100 nm, were used to prepare Nafion/Na-X zeolite composite membranes by recast method. The physical, chemical, and morphological properties of the zeolite powders and composite membranes were examined by XRD, N2 adsorption isotherms, FTIR, SEM, and SAXS analysis. Furthermore, the effect of zeolite particles size and loadings (i.e., 5 and 10% w/w) on the water, methanol, and proton transport properties was investigated.It has been found that the size of the Na-X zeolite particles plays a key role in the proton and methanol transport behavior since it rules the zeolite hydrophilic behavior, the morphology of polymer–filler interphase, and also the nature of water established in the composite membrane.The results show that the membranes loaded with a 5% w/w of submicron-sized Na-X zeolite exhibit a proton conductivity and selectivity significantly higher than Nafion. In particular the proton conductivity at 120 °C is around eight times and the selectivity at 25 °C is around 40% higher than those exhibited by recast Nafion.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201000172" xmlns="http://purl.org/rss/1.0/"><title>Water Management in A PEMFC: Water Transport Mechanism and Material Degradation in Gas Diffusion Layers</title><link>http://dx.doi.org/10.1002%2Ffuce.201000172</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Water Management in A PEMFC: Water Transport Mechanism and Material Degradation in Gas Diffusion Layers</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. G. Kandlikar</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. L. Garofalo</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Z. Lu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201000172</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/">10.1002/fuce.201000172</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201000172</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">814</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">823</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>It has now been well recognized that both the performance and durability of proton exchange membrane fuel cells (PEMFCs) are closely related to the water accumulation and transport inside its porous components, particularly in the gas diffusion layer (GDL), and microporous layer (MPL). In this paper, the key GDL and MPL properties that affect water transport through them are first discussed and a review of GDL degradation mechanisms is presented. An intermittent water drainage mechanism across the GDL is discussed. The capillary breakthrough pressure (CBP) and the dynamic capillary pressure (DCP), or recurrent breakthrough dynamics, have been identified as key GDL properties that affect its water management performance and function as indicators of the degradation of GDL material. This work uses a novel <em>ex situ</em> experiment to degrade a GDL by exposing it to an accelerated stress test (AST) that subjects the GDL to elevated operation conditions seen at the cathode side of a PEMFC for an extended period of time. In turn, the effect of the AST on the CBP and DCP is investigated. As a result, a loss of hydrophobicity occurred on the MPL surface. This altered the CBP and DCP, thus decreasing water management in the GDL.</p></div>]]></content:encoded><description>It has now been well recognized that both the performance and durability of proton exchange membrane fuel cells (PEMFCs) are closely related to the water accumulation and transport inside its porous components, particularly in the gas diffusion layer (GDL), and microporous layer (MPL). In this paper, the key GDL and MPL properties that affect water transport through them are first discussed and a review of GDL degradation mechanisms is presented. An intermittent water drainage mechanism across the GDL is discussed. The capillary breakthrough pressure (CBP) and the dynamic capillary pressure (DCP), or recurrent breakthrough dynamics, have been identified as key GDL properties that affect its water management performance and function as indicators of the degradation of GDL material. This work uses a novel ex situ experiment to degrade a GDL by exposing it to an accelerated stress test (AST) that subjects the GDL to elevated operation conditions seen at the cathode side of a PEMFC for an extended period of time. In turn, the effect of the AST on the CBP and DCP is investigated. As a result, a loss of hydrophobicity occurred on the MPL surface. This altered the CBP and DCP, thus decreasing water management in the GDL.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100086" xmlns="http://purl.org/rss/1.0/"><title>Uncertainties of Yeast-Based Biofuel Cell Operational Characteristics</title><link>http://dx.doi.org/10.1002%2Ffuce.201100086</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Uncertainties of Yeast-Based Biofuel Cell Operational Characteristics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Babanova</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Y. Hubenova</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. Mitov</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">P. Mandjukov</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100086</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/">10.1002/fuce.201100086</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100086</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">824</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">837</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The commonly used parameters characterizing fuel cells and in particular microbial fuel cells (MFCs) electrical performance are open circuit voltage (OCV), maximum power, and short circuit current. These characteristics are usually obtained from polarization and power curves. In the present study, the expanded uncertainties of operational characteristics for yeast-based fuel cell were evaluated and the main sources of uncertainty were determined. Two approaches were used: the uncertainty budget building for sources uncertainty estimation and a statistical treatment of identical MFCs results – for operational characteristics uncertainty calculation. It was found that in this particular bioelectrochemical system the major factor contributing to operational characteristics uncertainties was the electrodes' resistance. The operational characteristics uncertainties were decreased from 19 to 13% for OCV, from 42 to 14% for maximal power, and from 46 to 13% for short circuit current with the usage of electrodes with resistance in the interval 6–7 Ω. The described approaches can be used for operational characteristics expanded uncertainties calculation of all types of fuel cells using data from polarization measurements.</p></div>]]></content:encoded><description>The commonly used parameters characterizing fuel cells and in particular microbial fuel cells (MFCs) electrical performance are open circuit voltage (OCV), maximum power, and short circuit current. These characteristics are usually obtained from polarization and power curves. In the present study, the expanded uncertainties of operational characteristics for yeast-based fuel cell were evaluated and the main sources of uncertainty were determined. Two approaches were used: the uncertainty budget building for sources uncertainty estimation and a statistical treatment of identical MFCs results – for operational characteristics uncertainty calculation. It was found that in this particular bioelectrochemical system the major factor contributing to operational characteristics uncertainties was the electrodes' resistance. The operational characteristics uncertainties were decreased from 19 to 13% for OCV, from 42 to 14% for maximal power, and from 46 to 13% for short circuit current with the usage of electrodes with resistance in the interval 6–7 Ω. The described approaches can be used for operational characteristics expanded uncertainties calculation of all types of fuel cells using data from polarization measurements.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100090" xmlns="http://purl.org/rss/1.0/"><title>Experimental Characterization and Numerical Modeling of PEMFC Stacks Designed for Different Application Fields</title><link>http://dx.doi.org/10.1002%2Ffuce.201100090</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Experimental Characterization and Numerical Modeling of PEMFC Stacks Designed for Different Application Fields</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">E. Jannelli</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. Minutillo</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A. Perna</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100090</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/">10.1002/fuce.201100090</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100090</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">838</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">849</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Proton exchange membrane fuel cell (PEMFC) is regarded as a potential future power technology for stationary and mobile applications due to its high efficiency (full and partial load), rapid start-up, high power density, and low emissions.</p></div><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Depending on their particular application field (decentralized combined heat and power production, uninterrupted power supplies (UPS), or mobile applications) different operating conditions and designing parameters are required and different performance can be expected.</p></div><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Thus, the aim of this paper is to investigate the behavior and performance of two stacks of the same size, developed with a different approach according to their application sectors.</p></div><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The first PEMFC stack is designed for UPS units or mobile purpose, the second one, is designed to supply heat and power in residential applications (CHP units).</p></div><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The analysis of the stacks behavior has been carried out by using both experimental and numerical investigations.</p></div><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Experimental results have allowed: (i) to characterize the stacks; (ii) to calibrate the numerical model; (iii) to supply useful data for setting and improving the control system.</p></div>]]></content:encoded><description>Proton exchange membrane fuel cell (PEMFC) is regarded as a potential future power technology for stationary and mobile applications due to its high efficiency (full and partial load), rapid start-up, high power density, and low emissions.Depending on their particular application field (decentralized combined heat and power production, uninterrupted power supplies (UPS), or mobile applications) different operating conditions and designing parameters are required and different performance can be expected.Thus, the aim of this paper is to investigate the behavior and performance of two stacks of the same size, developed with a different approach according to their application sectors.The first PEMFC stack is designed for UPS units or mobile purpose, the second one, is designed to supply heat and power in residential applications (CHP units).The analysis of the stacks behavior has been carried out by using both experimental and numerical investigations.Experimental results have allowed: (i) to characterize the stacks; (ii) to calibrate the numerical model; (iii) to supply useful data for setting and improving the control system.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100036" xmlns="http://purl.org/rss/1.0/"><title>Investigating Reliability on Fuel Cell Model Identification. Part I: A Design of Experiments Approach</title><link>http://dx.doi.org/10.1002%2Ffuce.201100036</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Investigating Reliability on Fuel Cell Model Identification. Part I: A Design of Experiments Approach</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">L. Tsikonis</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. Van herle</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">D. Favrat</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100036</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/">10.1002/fuce.201100036</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100036</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">850</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">865</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>A model-based Design of Experiments method was employed for the optimization of measurements on a solid oxide fuel cell (SOFC). Based on a simplified SOFC model, a variation of the D-optimality was used as optimization criterion for the calculation of optimal experimental designs (determinant of the covariance matrix with weighting factors). Solutions for different numbers of design points were calculated and the behavior of optimization criteria as functions of the number of design points as well as of the number of repetitions of measurements was analyzed. A new type of graph was introduced which depicts the behavior of optimization criteria for constant number of measurements. This approach showed that, for constant numbers of measurements, the precision is higher and therefore the reliability in the cell's model identification is improved when repeated measurements of a small set of optimal design points are effectuated, instead of many different measurements. Finally, a sensitivity analysis was performed showing the influence of the parameter values on the values of the optimization criterion and the optimal measurements.</p></div><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The used methodology and its theoretical conclusions may be used as a basis for development of diagnostics tools or filtering existing data for optimal parameter estimations.</p></div>]]></content:encoded><description>A model-based Design of Experiments method was employed for the optimization of measurements on a solid oxide fuel cell (SOFC). Based on a simplified SOFC model, a variation of the D-optimality was used as optimization criterion for the calculation of optimal experimental designs (determinant of the covariance matrix with weighting factors). Solutions for different numbers of design points were calculated and the behavior of optimization criteria as functions of the number of design points as well as of the number of repetitions of measurements was analyzed. A new type of graph was introduced which depicts the behavior of optimization criteria for constant number of measurements. This approach showed that, for constant numbers of measurements, the precision is higher and therefore the reliability in the cell's model identification is improved when repeated measurements of a small set of optimal design points are effectuated, instead of many different measurements. Finally, a sensitivity analysis was performed showing the influence of the parameter values on the values of the optimization criterion and the optimal measurements.The used methodology and its theoretical conclusions may be used as a basis for development of diagnostics tools or filtering existing data for optimal parameter estimations.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100034" xmlns="http://purl.org/rss/1.0/"><title>Durability of Polymer Electrolyte Membrane Fuel Cell with Pt/CNTs Catalysts in Cell Reversal Conditions by Hydrogen Starvation</title><link>http://dx.doi.org/10.1002%2Ffuce.201100034</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Durability of Polymer Electrolyte Membrane Fuel Cell with Pt/CNTs Catalysts in Cell Reversal Conditions by Hydrogen Starvation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">D.-W. Jung</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Park</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S.-H. Kim</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J.-B. Kim</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">E.-S. Oh</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100034</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/">10.1002/fuce.201100034</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100034</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">866</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">874</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The durability of polymer electrolyte membrane fuel cell with Pt catalysts supported on carbon nanotube (CNT) was investigated after a few hundred accelerated cell reversal process (RP) cycles generated by hydrogen deficiency. A variety of characterization techniques, including cell performance tests, were applied to examine the effects of CNT support on the degradation of Pt catalysts: transmission electron microscopy, electrochemical impedance spectroscopy, and cyclic voltammetry. During the RP cycle tests, most degradation by carbon corrosion occurred at the outlet region of membrane electrode assembly (MEA) where hydrogen starvation seriously occurred. By using the CNT as the support of Pt catalysts in the MEA cathode, carbon corrosion was reduced and growth of Pt particles by agglomeration and sintering significantly decreased. Compared to a commercial Pt/C catalyst, the cell durability of the Pt/CNT catalyst was enhanced under the RP condition.</p></div>]]></content:encoded><description>The durability of polymer electrolyte membrane fuel cell with Pt catalysts supported on carbon nanotube (CNT) was investigated after a few hundred accelerated cell reversal process (RP) cycles generated by hydrogen deficiency. A variety of characterization techniques, including cell performance tests, were applied to examine the effects of CNT support on the degradation of Pt catalysts: transmission electron microscopy, electrochemical impedance spectroscopy, and cyclic voltammetry. During the RP cycle tests, most degradation by carbon corrosion occurred at the outlet region of membrane electrode assembly (MEA) where hydrogen starvation seriously occurred. By using the CNT as the support of Pt catalysts in the MEA cathode, carbon corrosion was reduced and growth of Pt particles by agglomeration and sintering significantly decreased. Compared to a commercial Pt/C catalyst, the cell durability of the Pt/CNT catalyst was enhanced under the RP condition.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100025" xmlns="http://purl.org/rss/1.0/"><title>Dynamic Thermal, Transport and Mechanical Model of Fuel Cell Membrane Swelling</title><link>http://dx.doi.org/10.1002%2Ffuce.201100025</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Dynamic Thermal, Transport and Mechanical Model of Fuel Cell Membrane Swelling</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">T. J. Silverman</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. P. Meyers</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. J. Beaman</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100025</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/">10.1002/fuce.201100025</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100025</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">875</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">887</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>When polymer electrolyte membrane materials are exposed to liquid water, they swell and distort. This frustrates the process of depositing liquid catalyst ink directly onto the membrane. We present a model predicting the transient compositional, thermal, and mechanical response of a membrane undergoing changes in water content. The model describes coupled heat and mass transfer and solid mechanics and is capable of describing the large changes in size and shape exhibited by a swelling membrane. Simulation results are presented for sorption and desorption and for the process of drying a saturated piece of membrane with an aqueous coating applied. We suggest that the well-established discrepancy in the rate of sorption and desorption may be partially due to pressure-driven diffusion effects absent in other models but present in ours. We also demonstrate that the model can represent the transient curling behavior of a membrane undergoing nonuniform changes in water content. The model will later be used to predict manufacturing defects caused by swelling-induced wrinkling.</p></div>]]></content:encoded><description>When polymer electrolyte membrane materials are exposed to liquid water, they swell and distort. This frustrates the process of depositing liquid catalyst ink directly onto the membrane. We present a model predicting the transient compositional, thermal, and mechanical response of a membrane undergoing changes in water content. The model describes coupled heat and mass transfer and solid mechanics and is capable of describing the large changes in size and shape exhibited by a swelling membrane. Simulation results are presented for sorption and desorption and for the process of drying a saturated piece of membrane with an aqueous coating applied. We suggest that the well-established discrepancy in the rate of sorption and desorption may be partially due to pressure-driven diffusion effects absent in other models but present in ours. We also demonstrate that the model can represent the transient curling behavior of a membrane undergoing nonuniform changes in water content. The model will later be used to predict manufacturing defects caused by swelling-induced wrinkling.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100041" xmlns="http://purl.org/rss/1.0/"><title>Effects of Humidification on the Membrane Electrode Assembly of Proton Exchange Membrane Fuel Cells at Relatively High Cell Temperatures</title><link>http://dx.doi.org/10.1002%2Ffuce.201100041</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effects of Humidification on the Membrane Electrode Assembly of Proton Exchange Membrane Fuel Cells at Relatively High Cell Temperatures</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">K.-M. Yin</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">C.-P. Chang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100041</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/">10.1002/fuce.201100041</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100041</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">888</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">896</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>This study focuses on the performances of proton exchange membrane fuel cells (PEMFCs) at 80 and 90 °C with feeds of varying degrees of humidification. The results show that ohmic resistance of the solid electrolyte decreases as the current density is raised because of the back diffusion of liquid water, that is, generated in the cathode active layer. On the other hand, severe liquid water accumulation occurs at high current densities, which hinders the oxygen transport in the cathode gas diffusion layer (GDL) resulting in the Nernst diffusion limitation. The polarization measurement correlates well with the electrochemical impedance spectroscopy (EIS) analysis. The effects of humidification on membrane hydration, activity in the catalyst layer, and oxygen diffusion over-potential in the cathode GDL are elucidated with the proposed equivalent circuit model at varying operating current densities.</p></div>]]></content:encoded><description>This study focuses on the performances of proton exchange membrane fuel cells (PEMFCs) at 80 and 90 °C with feeds of varying degrees of humidification. The results show that ohmic resistance of the solid electrolyte decreases as the current density is raised because of the back diffusion of liquid water, that is, generated in the cathode active layer. On the other hand, severe liquid water accumulation occurs at high current densities, which hinders the oxygen transport in the cathode gas diffusion layer (GDL) resulting in the Nernst diffusion limitation. The polarization measurement correlates well with the electrochemical impedance spectroscopy (EIS) analysis. The effects of humidification on membrane hydration, activity in the catalyst layer, and oxygen diffusion over-potential in the cathode GDL are elucidated with the proposed equivalent circuit model at varying operating current densities.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100004" xmlns="http://purl.org/rss/1.0/"><title>On the Methanol Permeability through Pristine Nafion® and Nafion/PVA Membranes Measured by Different Techniques. A Comparison of Methodologies</title><link>http://dx.doi.org/10.1002%2Ffuce.201100004</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">On the Methanol Permeability through Pristine Nafion® and Nafion/PVA Membranes Measured by Different Techniques. A Comparison of Methodologies</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Mollá</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">V. Compañ</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Luis Lafuente</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. Prats</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100004</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/">10.1002/fuce.201100004</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100004</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">897</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">906</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Methanol crossover through polymer electrolyte membranes is a critical issue and causes an important reduction of performance in direct methanol fuel cells (DMFCs). Measuring the evolution of CO<sub>2</sub> gas in the cathode is a common method to determine the methanol crossover under real operating conditions, although an easier and simpler method is preferable for the screening of membranes during their step of development. In this sense, this work has been focused on the <em>ex situ</em> characterization of the methanol permeability in novel nanofiber-reinforced composite Nafion/PVA membranes for DMFC application by means of three different experimental procedures: (a) potentiometric method, (b) gas chromatography technique, and (c) measuring the density. It was found that all these methods resulted in comparable results and it was observed that the incorporation of the PVA nanofiber phase within the Nafion® matrix causes a remarkable reduction of the methanol permeability. The optimal choice of the most suitable technique depends on the accuracy expected for the methanol concentration, the availability of the required instrumental, and the complexity of the procedure.</p></div>]]></content:encoded><description>Methanol crossover through polymer electrolyte membranes is a critical issue and causes an important reduction of performance in direct methanol fuel cells (DMFCs). Measuring the evolution of CO2 gas in the cathode is a common method to determine the methanol crossover under real operating conditions, although an easier and simpler method is preferable for the screening of membranes during their step of development. In this sense, this work has been focused on the ex situ characterization of the methanol permeability in novel nanofiber-reinforced composite Nafion/PVA membranes for DMFC application by means of three different experimental procedures: (a) potentiometric method, (b) gas chromatography technique, and (c) measuring the density. It was found that all these methods resulted in comparable results and it was observed that the incorporation of the PVA nanofiber phase within the Nafion® matrix causes a remarkable reduction of the methanol permeability. The optimal choice of the most suitable technique depends on the accuracy expected for the methanol concentration, the availability of the required instrumental, and the complexity of the procedure.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100017" xmlns="http://purl.org/rss/1.0/"><title>Electrocatalytic Performance of Pd Nanoparticles Supported on SiC Nanowires for Methanol Oxidation in Alkaline Media</title><link>http://dx.doi.org/10.1002%2Ffuce.201100017</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Electrocatalytic Performance of Pd Nanoparticles Supported on SiC Nanowires for Methanol Oxidation in Alkaline Media</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">X. Tong</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">L. Dong</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">G. Jin</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Y. Wang</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">X.-Y. Guo</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100017</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/">10.1002/fuce.201100017</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100017</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">907</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">910</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Pd nanoparticles (NPs) with a mean size of 10–12 nm are dispersed on the surface of SiC nanowires (NWs) by a cyclic voltammetric deposition method, and employed as an electrocatalyst for methanol oxidation. The high dispersion and small size of supported Pd NPs enable the catalyst to have an electrochemical active surface area of 49.5 m<sup>2</sup> g<sup>–1</sup>, which is larger than that of carbon nanotube supported Pd NPs (38.6 m<sup>2</sup> g<sup>–1</sup>), and that of non-supported Pd NPs (29.9 m<sup>2</sup> g<sup>–1</sup>). Methanol oxidation measurements show that the supported Pd NPs possess a high electrocatalytic activity and an excellent stability. These results indicate that SiC NWs have great potentials as an advantageous supporting material in alcohol fuel cells.</p></div>]]></content:encoded><description>Pd nanoparticles (NPs) with a mean size of 10–12 nm are dispersed on the surface of SiC nanowires (NWs) by a cyclic voltammetric deposition method, and employed as an electrocatalyst for methanol oxidation. The high dispersion and small size of supported Pd NPs enable the catalyst to have an electrochemical active surface area of 49.5 m2 g–1, which is larger than that of carbon nanotube supported Pd NPs (38.6 m2 g–1), and that of non-supported Pd NPs (29.9 m2 g–1). Methanol oxidation measurements show that the supported Pd NPs possess a high electrocatalytic activity and an excellent stability. These results indicate that SiC NWs have great potentials as an advantageous supporting material in alcohol fuel cells.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100012" xmlns="http://purl.org/rss/1.0/"><title>HT-PEM Fuel Cell System with Integrated Complex Metal Hydride Storage Tank</title><link>http://dx.doi.org/10.1002%2Ffuce.201100012</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">HT-PEM Fuel Cell System with Integrated Complex Metal Hydride Storage Tank</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">R. Urbanczyk</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Peil</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">D. Bathen</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">C. Heßke</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. Burfeind</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">K. Hauschild</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. Felderhoff</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">F. Schüth</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100012</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/">10.1002/fuce.201100012</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100012</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">911</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">920</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>A hydrogen storage tank based on the metal hydride sodium alanate is coupled with a high temperature PEM fuel cell (HT-PEM). The waste heat of the fuel cell is used for desorbing hydrogen from the storage tank that in return feeds the fuel cell. ZBT has developed the HT-PEM fuel cell, Max-Planck-Institut für Kohlenforschung the sodium alanate, and IUTA the hydrogen storage tank. During the experiments of the system the fuel cell was operated by load cycling from 165 up to 240 W. Approximately 60 g of hydrogen were delivered from the tank, which was charged with 2676.8 g of sodium alanate doped with 4 mol.% of TiCl<sub>3</sub>. This amount of hydrogen was desorbed in 3 h and generated a cumulated electrical energy of 660 Wh. In the first cycle 81.5 g of hydrogen were supplied during 3.69 h to the HT-PEM fuel cell, which was operated nearly constant at 260 W. In the latter case the cumulated electrical energy was 941 Wh.</p></div>]]></content:encoded><description>A hydrogen storage tank based on the metal hydride sodium alanate is coupled with a high temperature PEM fuel cell (HT-PEM). The waste heat of the fuel cell is used for desorbing hydrogen from the storage tank that in return feeds the fuel cell. ZBT has developed the HT-PEM fuel cell, Max-Planck-Institut für Kohlenforschung the sodium alanate, and IUTA the hydrogen storage tank. During the experiments of the system the fuel cell was operated by load cycling from 165 up to 240 W. Approximately 60 g of hydrogen were delivered from the tank, which was charged with 2676.8 g of sodium alanate doped with 4 mol.% of TiCl3. This amount of hydrogen was desorbed in 3 h and generated a cumulated electrical energy of 660 Wh. In the first cycle 81.5 g of hydrogen were supplied during 3.69 h to the HT-PEM fuel cell, which was operated nearly constant at 260 W. In the latter case the cumulated electrical energy was 941 Wh.</description></item><item rdf:about="http://dx.doi.org/10.1002%2Ffuce.201100024" xmlns="http://purl.org/rss/1.0/"><title>Sulfonated Aromatic Polyethers Containing Pyridine Units as Electrolytes for High Temperature Fuel Cells</title><link>http://dx.doi.org/10.1002%2Ffuce.201100024</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Sulfonated Aromatic Polyethers Containing Pyridine Units as Electrolytes for High Temperature Fuel Cells</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">I. Kalamaras</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. K. Daletou</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">V. G. Gregoriou</dc:creator><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. K. Kallitsis</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-01T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/fuce.201100024</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/">10.1002/fuce.201100024</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://dx.doi.org/10.1002%2Ffuce.201100024</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Research Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">921</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">931</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Novel sulfonated copolymers bearing main chain pyridine units have been synthesized for use as electrolytes in high temperature proton exchange membrane fuel cells (PEMFCs). The aim was to combine the excellent thermomechanical properties and high conductivity values after doping with phosphoric acid of these materials with the ability of the sulfonic groups to absorb and retain water and finally to examine the effect on the proton conduction ability. The resulted copolymers showed excellent film forming properties, mechanical integrity, and high glass transition temperatures (<em>T</em><sub>g</sub> &gt; 300 °C). The <em>T</em><sub>g</sub> of the sulfonated copolymers is strongly affected by the sulfonated group content in the polymer backbone due to the acid base interactions of the pyridine and sulfonated groups. Furthermore, the membranes exhibited remarkable oxidative stability and presented proton conductivities in the range of 10<sup>–2</sup> S cm<sup>–1</sup>.</p></div>]]></content:encoded><description>Novel sulfonated copolymers bearing main chain pyridine units have been synthesized for use as electrolytes in high temperature proton exchange membrane fuel cells (PEMFCs). The aim was to combine the excellent thermomechanical properties and high conductivity values after doping with phosphoric acid of these materials with the ability of the sulfonic groups to absorb and retain water and finally to examine the effect on the proton conduction ability. The resulted copolymers showed excellent film forming properties, mechanical integrity, and high glass transition temperatures (Tg &gt; 300 °C). The Tg of the sulfonated copolymers is strongly affected by the sulfonated group content in the polymer backbone due to the acid base interactions of the pyridine and sulfonated groups. Furthermore, the membranes exhibited remarkable oxidative stability and presented proton conductivities in the range of 10–2 S cm–1.</description></item></rdf:RDF>
