<?xml version="1.0" encoding="UTF-8"?>
<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)1939-019X" xmlns="http://purl.org/rss/1.0/"><title>The Canadian Journal of Chemical Engineering</title><description> Wiley Online Library : The Canadian Journal of Chemical Engineering</description><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2F%28ISSN%291939-019X</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  2013 Canadian Society for Chemical Engineering</dc:rights><prism:issn xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">0008-4034</prism:issn><prism:eIssn xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1939-019X</prism:eIssn><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-06-01T00:00:00-05:00</dc:date><prism:coverDisplayDate xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">June 2013</prism:coverDisplayDate><prism:volume xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">91</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/">1001</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1199</prism:endingPage><image rdf:resource="http://onlinelibrary.wiley.com/store/10.1002/cjce.v91.6/asset/cover.gif?v=1&amp;s=33bb15e3a48bf8dd20e2d12d97a507aa5e03108e"/><items><rdf:Seq><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21805"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21847"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21842"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21828"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21792"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21830"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21825"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21831"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21835"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21834"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21833"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21832"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21826"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21798"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21824"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21808"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21795"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21827"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21761"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21793"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21818"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21819"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21804"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21773"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21821"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21823"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21812"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21814"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21815"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21816"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21810"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21809"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21806"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21811"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21771"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21799"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21800"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21801"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21802"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21797"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21794"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21765"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21760"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21785"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21788"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21781"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21783"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21758"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21786"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21789"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21787"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21790"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21784"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21779"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21776"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21778"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21769"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21772"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21774"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21775"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21766"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21770"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21767"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21768"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21762"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21763"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21741"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21747"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21746"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21750"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21744"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21743"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21737"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21739"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21718"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21632"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.20388"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.20476"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21813"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21734"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21756"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21817"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21729"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21725"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21717"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21720"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21721"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21735"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21803"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21742"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21712"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21751"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21807"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21752"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21740"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21715"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21727"/></rdf:Seq></items></channel><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21805" xmlns="http://purl.org/rss/1.0/"><title>From molecules to processes: Molecular simulations applied to the design of simulated moving bed for ethane/ethylene separation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21805</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">From molecules to processes: Molecular simulations applied to the design of simulated moving bed for ethane/ethylene separation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Miguel Angelo Granato, Vanessa Duarte Martins, João Carlos Santos, Miguel Jorge, Alírio Egídio Rodrigues</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-17T11:36:51.406084-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21805</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21805</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21805</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separation Processes</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="section" id="cjce21805-sec-0001" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p>This paper presents results of a modelling study on the separation of ethane/ethylene mixture by selective adsorption on zeolite 13X in a simulated moving bed (SMB) unit. Propane and <em>n</em>-butane are evaluated as desorbent candidates. The study encompasses molecular simulation calculations for determination of adsorption parameters, whose results will then be used in a mathematical model for evaluating the performance of an SMB unit. This work is entirely done <em>in silico</em>, by using available force field parameters for the molecular simulations part and reliable mathematical models for the SMB part. Experimental data are solely used for comparison with the molecular simulation results, which are subsequently expanded to calculate adsorption properties for separating the mixtures, without further experimental work. The separation regions of an SMB unit operating with zeolite 13X for ethane/ethylene separation, using propane and <em>n</em>-butane as desorbents, were obtained by simulation at 110 kPa and at four different temperatures: 298, 323, 348 and 373 K. For each desorbent, an operating point was selected, and the size of the required unit was presented for the complete separation of the two components of the mixture.</p></div></div>
]]></content:encoded><description>


This paper presents results of a modelling study on the separation of ethane/ethylene mixture by selective adsorption on zeolite 13X in a simulated moving bed (SMB) unit. Propane and n-butane are evaluated as desorbent candidates. The study encompasses molecular simulation calculations for determination of adsorption parameters, whose results will then be used in a mathematical model for evaluating the performance of an SMB unit. This work is entirely done in silico, by using available force field parameters for the molecular simulations part and reliable mathematical models for the SMB part. Experimental data are solely used for comparison with the molecular simulation results, which are subsequently expanded to calculate adsorption properties for separating the mixtures, without further experimental work. The separation regions of an SMB unit operating with zeolite 13X for ethane/ethylene separation, using propane and n-butane as desorbents, were obtained by simulation at 110 kPa and at four different temperatures: 298, 323, 348 and 373 K. For each desorbent, an operating point was selected, and the size of the required unit was presented for the complete separation of the two components of the mixture.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21847" xmlns="http://purl.org/rss/1.0/"><title>Hydrodynamics of a powder-particle spouted bed with bottom feeding of powders conveyed by spouting gas</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21847</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Hydrodynamics of a powder-particle spouted bed with bottom feeding of powders conveyed by spouting gas</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hiroshi Nagashima, Kazumi Suzukawa, Toshifumi Ishikura</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-15T23:52:25.962862-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21847</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21847</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21847</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Spouted Beds-Vancouver special issue section</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="section" id="cjce21847-sec-0001" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p>Hydrodynamics of a powder-particle spouted bed (PPSB) with bottom feeding of fine powders conveyed by spouting gas has been investigated. Feeding of fine powders caused an increase in bed pressure drop, especially when a cohesive powder was fed. The minimum spouting velocity decreased with increasing feed rate of fines until a critical value, above which slugging occurred. Also, the fines became difficult to elutriate out of the PPSB when using a cohesive powder smaller than 40 µm. The elutriation rate constant and the mean residence time of fines in this study almost agreed with those obtained by top feeding.</p></div></div>
]]></content:encoded><description>


Hydrodynamics of a powder-particle spouted bed (PPSB) with bottom feeding of fine powders conveyed by spouting gas has been investigated. Feeding of fine powders caused an increase in bed pressure drop, especially when a cohesive powder was fed. The minimum spouting velocity decreased with increasing feed rate of fines until a critical value, above which slugging occurred. Also, the fines became difficult to elutriate out of the PPSB when using a cohesive powder smaller than 40 µm. The elutriation rate constant and the mean residence time of fines in this study almost agreed with those obtained by top feeding.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21842" xmlns="http://purl.org/rss/1.0/"><title>CHARACTERISING RAG-FORMING SOLIDS</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21842</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">CHARACTERISING RAG-FORMING SOLIDS</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Morvarid Madjlessi Kupai, Fan Yang, David Harbottle, Kevin Moran, Jacob Masliyah, Zhenghe Xu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-15T11:40:13.484754-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21842</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21842</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21842</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Special Issue Article on Oil Sands 2012</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="section" id="cjce21842-sec-0001" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p>In oil sands froth treatment, an undesirable intermediate layer, often accumulates during the separation of water–oil emulsions. The layer referred to as rag layer is a complex mixture of water, oil, solids and interfacially active components. The presence of a rag layer has a detrimental impact on the separation of water and fine solids from diluted bitumen. The current study focuses on characterisation of solids from a rag layer forming stream of a naphthenic froth treatment plant in an attempt to understand the mechanism of rag layer formation. Through detailed characterisation of rag-forming and non-rag-forming solids, the mineralogy of solids and their contamination were shown to be critical to rag layer formation. The iron-based minerals such as siderite and pyrite were found to be enriched within the rag layer. Analysis of surface organic complexes confirms a high level of organic matter associated with these solids through the binding of carboxylic acid group with iron on solids, resulting in a surface hydrophobicity susceptible for rag layer formation.</p></div></div>
]]></content:encoded><description>


In oil sands froth treatment, an undesirable intermediate layer, often accumulates during the separation of water–oil emulsions. The layer referred to as rag layer is a complex mixture of water, oil, solids and interfacially active components. The presence of a rag layer has a detrimental impact on the separation of water and fine solids from diluted bitumen. The current study focuses on characterisation of solids from a rag layer forming stream of a naphthenic froth treatment plant in an attempt to understand the mechanism of rag layer formation. Through detailed characterisation of rag-forming and non-rag-forming solids, the mineralogy of solids and their contamination were shown to be critical to rag layer formation. The iron-based minerals such as siderite and pyrite were found to be enriched within the rag layer. Analysis of surface organic complexes confirms a high level of organic matter associated with these solids through the binding of carboxylic acid group with iron on solids, resulting in a surface hydrophobicity susceptible for rag layer formation.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21828" xmlns="http://purl.org/rss/1.0/"><title>ADVANCED SIMULATION OF TRANSIENT MULTIPHASE FLOW &amp; FLOW ASSURANCE IN THE OIL &amp; GAS INDUSTRY</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21828</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">ADVANCED SIMULATION OF TRANSIENT MULTIPHASE FLOW &amp; FLOW ASSURANCE IN THE OIL &amp; GAS INDUSTRY</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Djamel Lakehal</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-03T02:42:34.003328-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21828</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21828</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21828</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena, Fluid Dynamics and Thermodynamics</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="section" id="cjce21828-sec-0001" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p>We discuss here current computational trends (beyond Mechanistic 1D Models) related to transient multiphase flow and flow assurance problems in the oil and gas sector. The developments needed to bring advanced Computational fluid &amp; <em>Multiphase</em>-fluid dynamics (CFD &amp; C<em>M</em>FD) techniques and models to a mature stage will also be discussed. The contribution presents the possibilities offered today by these simulation technologies to treat complex, multiphase, multicomponent flow problems occurring in the gas and petroleum engineering in general. Examples of various degrees of sophistication will be presented, without focusing on the validation aspect as such. The models are briefly introduced (phase averages, N-phase, interface tracking, Lagrangian particle tracking and granular flow model).</p></div></div>
]]></content:encoded><description>


We discuss here current computational trends (beyond Mechanistic 1D Models) related to transient multiphase flow and flow assurance problems in the oil and gas sector. The developments needed to bring advanced Computational fluid &amp; Multiphase-fluid dynamics (CFD &amp; CMFD) techniques and models to a mature stage will also be discussed. The contribution presents the possibilities offered today by these simulation technologies to treat complex, multiphase, multicomponent flow problems occurring in the gas and petroleum engineering in general. Examples of various degrees of sophistication will be presented, without focusing on the validation aspect as such. The models are briefly introduced (phase averages, N-phase, interface tracking, Lagrangian particle tracking and granular flow model).

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21792" xmlns="http://purl.org/rss/1.0/"><title>MHD FLOW OF BLOOD THROUGH A DUALLY STENOSED ARTERY: EFFECTS OF VISCOSITY VARIATION, VARIABLE HEMATOCRIT AND VELOCITY-SLIP</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21792</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">MHD FLOW OF BLOOD THROUGH A DUALLY STENOSED ARTERY: EFFECTS OF VISCOSITY VARIATION, VARIABLE HEMATOCRIT AND VELOCITY-SLIP</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A. Sinha, J.C. Misra</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-01T08:15:48.894649-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21792</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21792</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21792</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Biotechnology, Biochemical and Biomedical Engineering</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="section" id="cjce21792-sec-0001" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p>Of concern in the paper is a study on blood flow through a porous segment of an artery subject to the action of an external magnetic field. Effects of viscosity variation and variable hematocrit as well as velocity-slip at the arterial wall have been duly taken care of in the study. A model has been developed to perform the study by using the principles of magnetohydrodynamics (MHD). The model has been analysed theoretically by employing suitable mathematical methods. Analytical expressions have been derived for the velocity, minute expenditure of blood (volumetric flow rate), wall shear stress and pressure gradient. The said physical variables are computed by using a specific set of values of the various parameters involved in the analysis. This serves as an illustration of the validity of the mathematical model developed in the paper. The computational results are presented graphically. The study also provides important insight into the effects of slip velocity on blood velocity, wall shear stress and pressure gradient. The study further shows that the flow of blood in a porous artery is significantly influenced by the action of an external magnetic field.</p></div></div>
]]></content:encoded><description>


Of concern in the paper is a study on blood flow through a porous segment of an artery subject to the action of an external magnetic field. Effects of viscosity variation and variable hematocrit as well as velocity-slip at the arterial wall have been duly taken care of in the study. A model has been developed to perform the study by using the principles of magnetohydrodynamics (MHD). The model has been analysed theoretically by employing suitable mathematical methods. Analytical expressions have been derived for the velocity, minute expenditure of blood (volumetric flow rate), wall shear stress and pressure gradient. The said physical variables are computed by using a specific set of values of the various parameters involved in the analysis. This serves as an illustration of the validity of the mathematical model developed in the paper. The computational results are presented graphically. The study also provides important insight into the effects of slip velocity on blood velocity, wall shear stress and pressure gradient. The study further shows that the flow of blood in a porous artery is significantly influenced by the action of an external magnetic field.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21830" xmlns="http://purl.org/rss/1.0/"><title>COMPUTATION OF THE TWO-PHASE FLOW PROPERTIES OF INTERMEDIATE-WET POROUS MEDIA: A PORE NETWORK APPROACH</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21830</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">COMPUTATION OF THE TWO-PHASE FLOW PROPERTIES OF INTERMEDIATE-WET POROUS MEDIA: A PORE NETWORK APPROACH</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Christos D. Tsakiroglou</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-30T11:10:57.083479-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21830</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21830</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21830</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena, Fluid Dynamics and Thermodynamics</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">000</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">000</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="section" id="cjce21830-sec-0001" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p>A pore-and-throat network including fractal-like roughness features along its surface is employed to simulate primary drainage and secondary imbibition by accounting for the quasistatic motion of menisci in pores and throats and varying the contact angle from 0° (strongly water-wet conditions) to 180° (strongly oil-wet conditions). The angle of sharpness of roughness features defines a range of contact angles within which the cross-section of the throat or pore is occupied completely by the one fluid and conditions of intermediate wettability are established. In contrast, outside this range, both fluids may coexist in a pore or throat. Such differences on the fluid distribution at the pore level affect strongly the capillary, electrical and hydraulic properties of the porous medium and are reflected in the capillary pressure, resistivity index and relative permeability curves. The simulator is used to calculate the aforementioned two-phase flow coefficients as the pore system transits from strongly water-wet or strongly oil-wet to intermediate-wet. The capillary pressure curves are always sensitive to the wetting state and the particular value of the contact angle. The relative permeability and resistivity index curves for secondary imbibition are grouped in families of curves which are sensitive mainly to the wetting state (water-wet, intermediate-wet/water-wet pores, intermediate-wet/oil-wet pores, oil-wet) rather than to the particular value of the contact angle.</p></div></div>
]]></content:encoded><description>


A pore-and-throat network including fractal-like roughness features along its surface is employed to simulate primary drainage and secondary imbibition by accounting for the quasistatic motion of menisci in pores and throats and varying the contact angle from 0° (strongly water-wet conditions) to 180° (strongly oil-wet conditions). The angle of sharpness of roughness features defines a range of contact angles within which the cross-section of the throat or pore is occupied completely by the one fluid and conditions of intermediate wettability are established. In contrast, outside this range, both fluids may coexist in a pore or throat. Such differences on the fluid distribution at the pore level affect strongly the capillary, electrical and hydraulic properties of the porous medium and are reflected in the capillary pressure, resistivity index and relative permeability curves. The simulator is used to calculate the aforementioned two-phase flow coefficients as the pore system transits from strongly water-wet or strongly oil-wet to intermediate-wet. The capillary pressure curves are always sensitive to the wetting state and the particular value of the contact angle. The relative permeability and resistivity index curves for secondary imbibition are grouped in families of curves which are sensitive mainly to the wetting state (water-wet, intermediate-wet/water-wet pores, intermediate-wet/oil-wet pores, oil-wet) rather than to the particular value of the contact angle.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21825" xmlns="http://purl.org/rss/1.0/"><title>ROBUST STABILITY ANALYSIS INSPIRED BY CLASSICAL STATISTICAL PRINCIPLES</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21825</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">ROBUST STABILITY ANALYSIS INSPIRED BY CLASSICAL STATISTICAL PRINCIPLES</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Nilton Silva, Heleno Bispo, Romildo Brito, João Manzi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-30T11:10:46.498002-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21825</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21825</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21825</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Process Control, Systems Engineering and Statistics</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="section" id="cjce21825-sec-0001" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p>An analysis was made of robust stability by estimating the robust confidence region for the roots of the characteristic Equation of a process, which uses a typical PID controller with auto-tuning. From standard statistical concepts, considerations on the statistical distance associated with the chi-square distribution were taken into account when establishing the methodology, which enabled the region of robust stability to be found. The results show the robust stability region for all eigenvalues of characteristic equation, thus demonstrating the ability of the procedure. The region of stability can be updated online, thus enabling the stability of the system to be continuously evaluated, with little computational effort.</p></div></div>
]]></content:encoded><description>


An analysis was made of robust stability by estimating the robust confidence region for the roots of the characteristic Equation of a process, which uses a typical PID controller with auto-tuning. From standard statistical concepts, considerations on the statistical distance associated with the chi-square distribution were taken into account when establishing the methodology, which enabled the region of robust stability to be found. The results show the robust stability region for all eigenvalues of characteristic equation, thus demonstrating the ability of the procedure. The region of stability can be updated online, thus enabling the stability of the system to be continuously evaluated, with little computational effort.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21831" xmlns="http://purl.org/rss/1.0/"><title>ENHANCED EXTRACTION of 2,3-BUTANEDIOL BY MEDLEY SOLVENT OF SALT AND n-BUTANOL FROM AQUEOUS SOLUTION</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21831</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">ENHANCED EXTRACTION of 2,3-BUTANEDIOL BY MEDLEY SOLVENT OF SALT AND n-BUTANOL FROM AQUEOUS SOLUTION</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yan-Yang Wu, Kui Chen, Jia-Wen Zhu, Bin Wu, Lijun Ji, Ya-Ling Shen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-29T01:53:20.572242-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21831</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21831</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21831</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separation Processes</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">000</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">000</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="section" id="cjce21831-sec-0001" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p>Enhanced extraction of 2,3-butanediol by adding salt into solvent <em>n</em>-butanol has been studied in this paper. Ternary phase diagrams for 2,3-butanediol + water + salt have been determined. The influences of phase ratio, type of salts and salt content on distribution coefficient and selectivity have also been investigated systematically. With phase ratio of 0.75 (w/w) and salt content of K<sub>2</sub>HPO<sub>4</sub> of 25% (w/w), the distribution coefficient, separation factors and recovery yield in a single extraction process by <em>n</em>-butanol can reach 5.2%, 34% and 80%, respectively. Salt addition can greatly enlarge the two phase region and enhance extraction simultaneously in this system.</p></div></div>
]]></content:encoded><description>


Enhanced extraction of 2,3-butanediol by adding salt into solvent n-butanol has been studied in this paper. Ternary phase diagrams for 2,3-butanediol + water + salt have been determined. The influences of phase ratio, type of salts and salt content on distribution coefficient and selectivity have also been investigated systematically. With phase ratio of 0.75 (w/w) and salt content of K2HPO4 of 25% (w/w), the distribution coefficient, separation factors and recovery yield in a single extraction process by n-butanol can reach 5.2%, 34% and 80%, respectively. Salt addition can greatly enlarge the two phase region and enhance extraction simultaneously in this system.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21835" xmlns="http://purl.org/rss/1.0/"><title>ROLE OF ASPHALTENES IN STABILISATION OF WATER IN CRUDE OIL EMULSIONS</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21835</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">ROLE OF ASPHALTENES IN STABILISATION OF WATER IN CRUDE OIL EMULSIONS</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jan Czarnecki, Plamen Tchoukov, Tadeusz Dabros, Zhenghe Xu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-26T09:15:32.419897-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21835</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21835</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21835</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Special Issue Article on Oil Sands 2012</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="section" id="cjce21835-sec-0001" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p>Even though asphaltenes do not have the well-defined amphiphilic structure characteristic of surfactants, it has been shown that they can stabilise water-in-oil emulsions. We propose that this stabilisation occurs because asphaltene aggregation results in the formation of a network within the thin oil film separating approaching emulsified water droplets. This network changes the rheology of the film to non-Newtonian, which prevents drainage of the film at thicknesses less than about 50–100 nm. The presence of the network also imparts steric stabilisation to the emulsion. The proposed stabilisation mechanism does not invoke any surfactant-like behaviour of asphaltenes. Instead, it relies solely on their propensity to aggregate.</p></div></div>
]]></content:encoded><description>


Even though asphaltenes do not have the well-defined amphiphilic structure characteristic of surfactants, it has been shown that they can stabilise water-in-oil emulsions. We propose that this stabilisation occurs because asphaltene aggregation results in the formation of a network within the thin oil film separating approaching emulsified water droplets. This network changes the rheology of the film to non-Newtonian, which prevents drainage of the film at thicknesses less than about 50–100 nm. The presence of the network also imparts steric stabilisation to the emulsion. The proposed stabilisation mechanism does not invoke any surfactant-like behaviour of asphaltenes. Instead, it relies solely on their propensity to aggregate.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21834" xmlns="http://purl.org/rss/1.0/"><title>INFLUENCE OF THE SECOND EMULSIFICATION STEP DURING PRODUCTION OF W/O/W MULTIPLE EMULSIONS: COMPARISON OF DIFFERENT METHODS TO DETERMINE ENCAPSULATION EFFICIENCY IN W/O/W EMULSIONS</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21834</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">INFLUENCE OF THE SECOND EMULSIFICATION STEP DURING PRODUCTION OF W/O/W MULTIPLE EMULSIONS: COMPARISON OF DIFFERENT METHODS TO DETERMINE ENCAPSULATION EFFICIENCY IN W/O/W EMULSIONS</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Anna Schuch, Ayse Nur Tonay, Karsten Köhler, Heike P. Schuchmann</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-26T08:57:09.35429-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21834</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21834</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21834</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Emulsification Special Issue Section</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">000</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">000</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="section" id="cjce21834-sec-0001" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p>As water encapsulation is crucial for most W/O/W emulsion applications, we compare different measurement techniques for its analysis. Therefore, we produce two different W/O/W emulsions that should have different EE, as we change the applied shear rate during the second emulsification step. We use the marker based techniques photometry (with Vitamin B12) and electroconductivity (using NaCl), rheometry as another indirect technique as well as DSC as a direct measurement method. It was found that photometry was not capable to detect differences between the emulsions. As DSC is the only direct technique, we conclude that it is most suitable to measure EE.</p></div></div>
]]></content:encoded><description>


As water encapsulation is crucial for most W/O/W emulsion applications, we compare different measurement techniques for its analysis. Therefore, we produce two different W/O/W emulsions that should have different EE, as we change the applied shear rate during the second emulsification step. We use the marker based techniques photometry (with Vitamin B12) and electroconductivity (using NaCl), rheometry as another indirect technique as well as DSC as a direct measurement method. It was found that photometry was not capable to detect differences between the emulsions. As DSC is the only direct technique, we conclude that it is most suitable to measure EE.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21833" xmlns="http://purl.org/rss/1.0/"><title>SOFT SENSOR SOLUTIONS FOR CONTROL OF OIL SANDS PROCESSES</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21833</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">SOFT SENSOR SOLUTIONS FOR CONTROL OF OIL SANDS PROCESSES</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Shima Khatibisepehr, Biao Huang, Elom Domlan, Elham Naghoosi, Yu Zhao, Yu Miao, Xinguang Shao, Swanand Khare, Marziyeh Keshavarz, Enbo Feng, Fangwei Xu, Aris Espejo, Ramesh Kadali</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-26T08:24:50.758599-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21833</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21833</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21833</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Special Issue Article on Oil Sands 2012</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">000</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">000</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="section" id="cjce21833-sec-0001" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p>Oil sands development is both a costly and technically complex business with potential concerns in land use, water consumption and greenhouse gas emissions. Therefore, it is of practical interest to further investigate novel techniques to improve profitability while diligently maintaining environmental compliance. Our approach for finding solutions to achieve this objective is to develop innovative strategies for advanced monitoring, optimisation and control of plant operations. Development of reliable process models is a key requirement for investigating the behaviour of complex systems. Such descriptive models can help to improve analysis, simulation, optimisation, design, control and operation of process systems at both micro and macro levels. This paper presents a summary of some of the successful applications focussed on development and implementation of inferential process models, also known as soft sensors for oil sands processes.</p></div></div>
]]></content:encoded><description>


Oil sands development is both a costly and technically complex business with potential concerns in land use, water consumption and greenhouse gas emissions. Therefore, it is of practical interest to further investigate novel techniques to improve profitability while diligently maintaining environmental compliance. Our approach for finding solutions to achieve this objective is to develop innovative strategies for advanced monitoring, optimisation and control of plant operations. Development of reliable process models is a key requirement for investigating the behaviour of complex systems. Such descriptive models can help to improve analysis, simulation, optimisation, design, control and operation of process systems at both micro and macro levels. This paper presents a summary of some of the successful applications focussed on development and implementation of inferential process models, also known as soft sensors for oil sands processes.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21832" xmlns="http://purl.org/rss/1.0/"><title>CATALYTIC GASIFICATION OF LIGNITE WITH KOH IN SUPERCRITICAL WATER</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21832</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">CATALYTIC GASIFICATION OF LIGNITE WITH KOH IN SUPERCRITICAL WATER</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Fenggao Xia, Senlin Tian, Ping Ning, Junjie Gu, Qingqing Guan, Rongrong Miao, Yixue Wang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-26T08:24:36.709293-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21832</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21832</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21832</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Environment, Renewable Resources and Green Processes</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">000</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">000</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="section" id="cjce21832-sec-0001" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p>Supercritical water gasification of lignite with KOH was investigated in a batch autoclave on a wide range of conditions, that is residence time (5–30 min), mass ratio of H<sub>2</sub>O to lignite (0.5–10), temperature (400–600°C) and mass ratio of KOH to lignite (0–20%). Although lignite is difficult to be gasified in supercritical water, the results indicated that gasification efficiency about 47% was achieved at 30 min, 550°C with 10% KOH. Higher mass ratio of H<sub>2</sub>O to lignite and temperature can lead to higher gas yields and GE. It is also observed that the solid residue was dispersed at low feed concentration and consolidated at high concentration. Besides KOH's improvement of water–gas shift reaction, in this case, it is also observed that KOH also enhances the gasification of aromatics of lignite in supercritical water, which leads to higher gasification efficiency of lignite.</p></div></div>
]]></content:encoded><description>


Supercritical water gasification of lignite with KOH was investigated in a batch autoclave on a wide range of conditions, that is residence time (5–30 min), mass ratio of H2O to lignite (0.5–10), temperature (400–600°C) and mass ratio of KOH to lignite (0–20%). Although lignite is difficult to be gasified in supercritical water, the results indicated that gasification efficiency about 47% was achieved at 30 min, 550°C with 10% KOH. Higher mass ratio of H2O to lignite and temperature can lead to higher gas yields and GE. It is also observed that the solid residue was dispersed at low feed concentration and consolidated at high concentration. Besides KOH's improvement of water–gas shift reaction, in this case, it is also observed that KOH also enhances the gasification of aromatics of lignite in supercritical water, which leads to higher gasification efficiency of lignite.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21826" xmlns="http://purl.org/rss/1.0/"><title>NUMERICAL MODELLING OF MICROWAVE HEATING OF FROZEN WOOD</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21826</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">NUMERICAL MODELLING OF MICROWAVE HEATING OF FROZEN WOOD</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">F. Erchiqui, Z. Annasabi, A. Koubaa, F. Slaoui-Hasnaoui, H. Kaddami</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-26T07:58:51.778864-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21826</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21826</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21826</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena, Fluid Dynamics and Thermodynamics</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="section" id="cjce21826-sec-0001" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p>The heating process of frozen wood exposed to plane microwaves is numerically investigated. The nonlinear heat conduction problem involving phase change such as wood freezing is solved by a specific 3D volumetric enthalpy-based finite element method. Dielectric and thermal properties are a function of temperature and moisture content. The numerical model is validated by experimental and analytical means. As an application, we studied the effect of moisture content and frequency on microwave heating of trembling aspen wood.</p></div></div>
]]></content:encoded><description>


The heating process of frozen wood exposed to plane microwaves is numerically investigated. The nonlinear heat conduction problem involving phase change such as wood freezing is solved by a specific 3D volumetric enthalpy-based finite element method. Dielectric and thermal properties are a function of temperature and moisture content. The numerical model is validated by experimental and analytical means. As an application, we studied the effect of moisture content and frequency on microwave heating of trembling aspen wood.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21798" xmlns="http://purl.org/rss/1.0/"><title>XYLANASE AND LACCASE AIDED BIO-BLEACHING OF WHEAT STRAW PULP</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21798</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">XYLANASE AND LACCASE AIDED BIO-BLEACHING OF WHEAT STRAW PULP</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Bhavin S. Dedhia, Mangesh D. Vetal, Virendra K. Rathod, Csoka Levente</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-26T04:05:50.226412-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21798</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21798</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21798</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separation Processes</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="section" id="cjce21798-sec-0001" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p>This paper illustrates the application of enzymes (e.g. xylanase and laccase) in the bio-bleaching of non-woody material (e.g. wheat straw). The objective of this paper is to develop an alternative bleaching sequence avoiding the use of chlorine during bleaching. In the study, wheat straw pulp has been treated with commercially available xylanase and laccase separately and sequentially. Optimised parameters for the xylanase pre-treatment are pH 5.5, temperature 60°C, enzyme dose 6 IU/g, pre-treatment time 75 min and speed of agitation 80 rpm. Similarly, optimum parameters for laccase delignification are pH 3.5, temperature 60°C, enzyme dose 22.5 IU/g of oven dried pulp, mediator concentration 1.5% of oven dried pulp (odp), delignification time 10 h and speed of agitation 120 rpm. On the other hand, sequential treatments such as xylanase pre-treatment (X) followed by laccase (L) and alkaline perdoxide (E) in presence of mediator have shown better reduction in kappa number, that is 24.84% as compared to LE in presence and absence of a mediator.</p></div></div>
]]></content:encoded><description>


This paper illustrates the application of enzymes (e.g. xylanase and laccase) in the bio-bleaching of non-woody material (e.g. wheat straw). The objective of this paper is to develop an alternative bleaching sequence avoiding the use of chlorine during bleaching. In the study, wheat straw pulp has been treated with commercially available xylanase and laccase separately and sequentially. Optimised parameters for the xylanase pre-treatment are pH 5.5, temperature 60°C, enzyme dose 6 IU/g, pre-treatment time 75 min and speed of agitation 80 rpm. Similarly, optimum parameters for laccase delignification are pH 3.5, temperature 60°C, enzyme dose 22.5 IU/g of oven dried pulp, mediator concentration 1.5% of oven dried pulp (odp), delignification time 10 h and speed of agitation 120 rpm. On the other hand, sequential treatments such as xylanase pre-treatment (X) followed by laccase (L) and alkaline perdoxide (E) in presence of mediator have shown better reduction in kappa number, that is 24.84% as compared to LE in presence and absence of a mediator.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21824" xmlns="http://purl.org/rss/1.0/"><title>A DUAL APPROACH FOR MODELLING AND OPTIMISATION OF INDUSTRIAL UREA REACTOR: SMART TECHNIQUE AND GREY BOX MODEL</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21824</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A DUAL APPROACH FOR MODELLING AND OPTIMISATION OF INDUSTRIAL UREA REACTOR: SMART TECHNIQUE AND GREY BOX MODEL</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sohrab Zendehboudi, Gholamreza Zahedi, Alireza Bahadori, Ali Lohi, Ali Elkamel, Ioannis Chatzis</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-26T04:05:42.918955-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21824</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21824</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21824</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Process Control, Systems Engineering and Statistics</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="section" id="cjce21824-sec-0001" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p>Urea has the highest demand among all solid nitrogenous fertilisers within the agriculture industry. In this paper, a mathematical model and an Artificial Neural Network (ANN) technique are proposed for the simulation and optimisation of the urea plant in an industrial petrochemical company. The developed mathematical model consists of complex vapour–liquid equilibria for the NH<sub>3</sub>–CO<sub>2</sub>–H<sub>2</sub>O–(NH<sub>2</sub>)<sub>2</sub>CO system in thermodynamic and reaction frameworks. The smart technique (e.g. ANN) considers the CO<sub>2</sub> conversion in terms of temperature and the molar ratios of NH<sub>3</sub>/CO<sub>2</sub> and H<sub>2</sub>O/CO<sub>2</sub> in the liquid phase. The ANN predictions were compared with the real data and results obtained from the mathematical model. An acceptable agreement was attained between deterministic methods. Through implementation of a systematic sensitivity analysis, it was found that a temperature of 191°C, a pressure of 132 atm and a NH<sub>3</sub>/CO<sub>2</sub> ratio of 2.7 are the optimum process conditions for the urea production. It is concluded that the developed ANN (or connectionist) technique is an efficient tool for modelling complex phase equilibria with reaction in the industrial urea plant.</p></div></div>
]]></content:encoded><description>


Urea has the highest demand among all solid nitrogenous fertilisers within the agriculture industry. In this paper, a mathematical model and an Artificial Neural Network (ANN) technique are proposed for the simulation and optimisation of the urea plant in an industrial petrochemical company. The developed mathematical model consists of complex vapour–liquid equilibria for the NH3–CO2–H2O–(NH2)2CO system in thermodynamic and reaction frameworks. The smart technique (e.g. ANN) considers the CO2 conversion in terms of temperature and the molar ratios of NH3/CO2 and H2O/CO2 in the liquid phase. The ANN predictions were compared with the real data and results obtained from the mathematical model. An acceptable agreement was attained between deterministic methods. Through implementation of a systematic sensitivity analysis, it was found that a temperature of 191°C, a pressure of 132 atm and a NH3/CO2 ratio of 2.7 are the optimum process conditions for the urea production. It is concluded that the developed ANN (or connectionist) technique is an efficient tool for modelling complex phase equilibria with reaction in the industrial urea plant.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21808" xmlns="http://purl.org/rss/1.0/"><title>A NOVEL MODIFICATION OF VAPOUR-LIFT LIQUID DISTRIBUTOR</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21808</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A NOVEL MODIFICATION OF VAPOUR-LIFT LIQUID DISTRIBUTOR</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Wei Du, Wenming Liu, Jian Xu, Weisheng Wei</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-26T04:05:23.36642-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21808</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21808</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21808</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, Chemical Kinetics and Catalysis</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="section" id="cjce21808-sec-0001" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p>For upgrading the liquid distribution in a trickle-bed reactor, the distributor is always the primary consideration. The vapour-lift tube device, most widely used in industry, still has disadvantages like mal-distribution to overcome. Therefore in this paper, two major modifications, that is increasing of slot numbers and opening side pores, were proposed to improve its liquid distribution performance. Cold-flow model tests were carried out with liquid distribution, and pressure drop was measured by liquid collectors and Omega pressure sensor, respectively. The results showed that as compared with proto type, the modified liquid distributor has a better liquid distribution performance and a lower pressure drop. Liquid distribution increases with the increasing of gas/liquid velocity ratio <em>ϵ</em> only when it is &lt;200. The pressure drop of new distributor increases with increasing of inner tube gas velocity and <em>ϵ</em>. Finally, correlations for liquid distribution and pressure drop of a new distributor were derived, showing rather good agreements with experimental results.</p></div></div>
]]></content:encoded><description>


For upgrading the liquid distribution in a trickle-bed reactor, the distributor is always the primary consideration. The vapour-lift tube device, most widely used in industry, still has disadvantages like mal-distribution to overcome. Therefore in this paper, two major modifications, that is increasing of slot numbers and opening side pores, were proposed to improve its liquid distribution performance. Cold-flow model tests were carried out with liquid distribution, and pressure drop was measured by liquid collectors and Omega pressure sensor, respectively. The results showed that as compared with proto type, the modified liquid distributor has a better liquid distribution performance and a lower pressure drop. Liquid distribution increases with the increasing of gas/liquid velocity ratio ϵ only when it is &lt;200. The pressure drop of new distributor increases with increasing of inner tube gas velocity and ϵ. Finally, correlations for liquid distribution and pressure drop of a new distributor were derived, showing rather good agreements with experimental results.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21795" xmlns="http://purl.org/rss/1.0/"><title>FAULT DETECTION AND DIAGNOSIS FOR DISTILLATION COLUMN USING TWO-TIER MODEL</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21795</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">FAULT DETECTION AND DIAGNOSIS FOR DISTILLATION COLUMN USING TWO-TIER MODEL</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Wen-De Tian, Su-Li Sun, Qing-Jie Guo</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-26T04:04:58.631678-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21795</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21795</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21795</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Process Control, Systems Engineering and Statistics</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="section" id="cjce21795-sec-0001" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p>In this paper, a two-tier model-based fault detection and diagnosis method for a distillation column is developed. It employs the nonlinear model developed earlier to monitor the distillation process and a corresponding linear model to identify an abnormal source when large deviations of measured values occur. The inner distillation fault parameters are estimated through linear least-square method based on the linear model. The proposed method is applied to the stripping tower in the Tennessee Eastman process simulator. Case studies demonstrate that the two-tier diagnosis structure effectively captures the variation of fault parameters and is more efficient than a pure nonlinear model-based structure.</p></div></div>
]]></content:encoded><description>


In this paper, a two-tier model-based fault detection and diagnosis method for a distillation column is developed. It employs the nonlinear model developed earlier to monitor the distillation process and a corresponding linear model to identify an abnormal source when large deviations of measured values occur. The inner distillation fault parameters are estimated through linear least-square method based on the linear model. The proposed method is applied to the stripping tower in the Tennessee Eastman process simulator. Case studies demonstrate that the two-tier diagnosis structure effectively captures the variation of fault parameters and is more efficient than a pure nonlinear model-based structure.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21827" xmlns="http://purl.org/rss/1.0/"><title>Decomposition of the most potent greenhouse gas (GHG) sulphur hexafluoride (SF6) using a dielectric barrier discharge (DBD) plasma</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21827</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Decomposition of the most potent greenhouse gas (GHG) sulphur hexafluoride (SF6) using a dielectric barrier discharge (DBD) plasma</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Quan Zhuang, Bruce Clements, Andrew McFarlan, Yemi Fasoyinu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-19T07:34:57.172641-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21827</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21827</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21827</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Environment, Renewable Resources and Green Processes</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 DBD method has been developed to decompose sulphur hexafluoride (SF<sub>6</sub>) nearly 100% under conditions close to the exhaust gas in industries with energy efficiency of 0.015–0.15 GJ/ton carbon dioxide (CO<sub>2</sub>) equivalent, 1–2 orders of magnitude higher than CO<sub>2</sub> capture and sequestration from power generation boilers. A typical test condition was SF<sub>6</sub>: 820 ppm; CO<sub>2</sub>/air: 50/50; gas flow rate: 623 mL/m at 25°C; AC voltage: 17–23 kV p–p; AC frequency: 7 kHz. The success of this project was due to the development of highly effective star-shaped discharge elements and an improved design of the DBD system, that is mode of applying voltage, the physical aspects of the reactor. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

A DBD method has been developed to decompose sulphur hexafluoride (SF6) nearly 100% under conditions close to the exhaust gas in industries with energy efficiency of 0.015–0.15 GJ/ton carbon dioxide (CO2) equivalent, 1–2 orders of magnitude higher than CO2 capture and sequestration from power generation boilers. A typical test condition was SF6: 820 ppm; CO2/air: 50/50; gas flow rate: 623 mL/m at 25°C; AC voltage: 17–23 kV p–p; AC frequency: 7 kHz. The success of this project was due to the development of highly effective star-shaped discharge elements and an improved design of the DBD system, that is mode of applying voltage, the physical aspects of the reactor. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21761" xmlns="http://purl.org/rss/1.0/"><title>Experimental evidence of low Rayleigh vibration on mixture during thermodiffusion experiment</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21761</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Experimental evidence of low Rayleigh vibration on mixture during thermodiffusion experiment</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Armin Kianian, Amirhossein Ahadi, M. Ziad Saghir</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-19T07:34:54.378141-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21761</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21761</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21761</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<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 paper demonstrates the influence of low Rayleigh vibration on thermodiffusion measurement in microgravity environment. The goal is to show how the variation of certain parameters such as frequency and amplitude of translational vibrations would impact the results obtained from the ISS experiment. Precisely, impact of change in low Rayleigh vibration on the separation of a component is studied for each experimental run.</p></div>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>ISS experimental data are obtained based on optical digital interferometry in a reduced gravity environment. The experiment is done in a cubic cell containing an aqueous solution exposed to a lateral temperature gradient. A mixture of water and isopropanol of different initial concentrations with positive and negative Soret coefficient is chosen as the test fluid. Collected data are analysed by image processing. Results show maximum separation of components for the case without any forced vibration. Moreover, an increase in Rayleigh number corresponds to decrease in the separation of components. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

This paper demonstrates the influence of low Rayleigh vibration on thermodiffusion measurement in microgravity environment. The goal is to show how the variation of certain parameters such as frequency and amplitude of translational vibrations would impact the results obtained from the ISS experiment. Precisely, impact of change in low Rayleigh vibration on the separation of a component is studied for each experimental run.
ISS experimental data are obtained based on optical digital interferometry in a reduced gravity environment. The experiment is done in a cubic cell containing an aqueous solution exposed to a lateral temperature gradient. A mixture of water and isopropanol of different initial concentrations with positive and negative Soret coefficient is chosen as the test fluid. Collected data are analysed by image processing. Results show maximum separation of components for the case without any forced vibration. Moreover, an increase in Rayleigh number corresponds to decrease in the separation of components. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21793" xmlns="http://purl.org/rss/1.0/"><title>Improved pre-treatment of porous stainless steel substrate for preparation of Pd-based composite membrane</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21793</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Improved pre-treatment of porous stainless steel substrate for preparation of Pd-based composite membrane</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Nong Xu, Shinkun Ryi, Anwu Li, John R. Grace, Jim Lim, Tony Boyd</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-18T09:50:58.187386-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21793</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21793</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21793</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separation Processes</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 integrity and robustness of Pd-based composite membranes depend heavily on the quality of the metallic substrate. This paper presents an improved method for pre-treating the substrate. Detailed pre-treatment steps of these porous stainless steel substrates included washing, polishing, etching, coating the first alumina layer, calcining the first alumina layer, coating the second alumina layer, calcining the second alumina layer and repair. The repair cycle was the most helpful step, greatly improving the membrane reproducibility and stability. Repeat coating with dilute suspensions of alumina particles of 0.3 µm mean diameter can repair defects on the top alumina layer. The hydrogen permeation flux was 268 × 10<sup>−4</sup> N m<sup>3</sup>/(m<sup>2</sup> h Pa) after one repair cycle, decreasing by 14% after an additional repair cycle. The hydrogen permeation flux of the pre-treated porous stainless steel substrate was thus maintained at a level comparable with previous work. Surface topography revealed that the average roughness was reduced from 1.15 to 0.47 µm, and the surface Maximum Peak to Valley decreased from 17.5 to 6.0 µm/mm<sup>2</sup> as a result of the pre-treatment. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

The integrity and robustness of Pd-based composite membranes depend heavily on the quality of the metallic substrate. This paper presents an improved method for pre-treating the substrate. Detailed pre-treatment steps of these porous stainless steel substrates included washing, polishing, etching, coating the first alumina layer, calcining the first alumina layer, coating the second alumina layer, calcining the second alumina layer and repair. The repair cycle was the most helpful step, greatly improving the membrane reproducibility and stability. Repeat coating with dilute suspensions of alumina particles of 0.3 µm mean diameter can repair defects on the top alumina layer. The hydrogen permeation flux was 268 × 10−4 N m3/(m2 h Pa) after one repair cycle, decreasing by 14% after an additional repair cycle. The hydrogen permeation flux of the pre-treated porous stainless steel substrate was thus maintained at a level comparable with previous work. Surface topography revealed that the average roughness was reduced from 1.15 to 0.47 µm, and the surface Maximum Peak to Valley decreased from 17.5 to 6.0 µm/mm2 as a result of the pre-treatment. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21818" xmlns="http://purl.org/rss/1.0/"><title>Understanding of no-load power in low consistency refiners</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21818</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Understanding of no-load power in low consistency refiners</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">N. Rajabi Nasab, J. A. Olson, J. Heymer, D. M. Martinez</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-18T09:50:56.255182-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21818</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21818</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21818</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena, Fluid Dynamics and Thermodynamics</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="section" id="cjce21818-sec-0001" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p>Low consistency refining is primary means of improving the paper quality by imparting energy to fibres through repeated fibre–bar interactions. Useful part of the energy modifies the morphology of fibres and the remaining, no-load power, overcomes the hydraulic, pumping and mechanical losses in the refiner. In this study, effect of consistency, operational and plate design parameters on no-load power was experimentally determined on two pilot scale refiners with different diameters. Obtained data were used to provide a statistical model for prediction of no-load power. To study the effect of diameter and groove depth, no-load power of some mills were collected.</p></div></div>
]]></content:encoded><description>


Low consistency refining is primary means of improving the paper quality by imparting energy to fibres through repeated fibre–bar interactions. Useful part of the energy modifies the morphology of fibres and the remaining, no-load power, overcomes the hydraulic, pumping and mechanical losses in the refiner. In this study, effect of consistency, operational and plate design parameters on no-load power was experimentally determined on two pilot scale refiners with different diameters. Obtained data were used to provide a statistical model for prediction of no-load power. To study the effect of diameter and groove depth, no-load power of some mills were collected.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21819" xmlns="http://purl.org/rss/1.0/"><title>Long-term statistical stability of industrial plants: Performance indicators and monitoring of an industrial pet plant</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21819</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Long-term statistical stability of industrial plants: Performance indicators and monitoring of an industrial pet plant</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Viviane Filgueiras, Enrique Luis Lima, José Carlos Pinto</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-18T09:50:54.952848-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21819</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21819</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21819</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Process Control, Systems Engineering and Statistics</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 the present work, usual statistical process control (SPC) definitions are reformulated to allow for long-term analyses, giving rise to extended statistical process control (ESPC) procedures. In order to allow for implementation of the ESPC approach, <em>t</em>- and <em>F</em>-control charts and monitoring indexes (NEPM, EPY and OEP) are designed in this work and are used to monitor the performance of a real industrial poly(ethylene terephthalate) (PET) site based on six process outputs (intrinsic viscosity, crystallinity, acetaldehyde concentration and colours a, b and L). As shown in this manuscript, ESPC tools allow for proper and systematic analysis of huge amounts of industrial data, using simple, fast and efficient statistical techniques, which can be used to improve the quality of the process operation in most industrial polymerisation plants. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

In the present work, usual statistical process control (SPC) definitions are reformulated to allow for long-term analyses, giving rise to extended statistical process control (ESPC) procedures. In order to allow for implementation of the ESPC approach, t- and F-control charts and monitoring indexes (NEPM, EPY and OEP) are designed in this work and are used to monitor the performance of a real industrial poly(ethylene terephthalate) (PET) site based on six process outputs (intrinsic viscosity, crystallinity, acetaldehyde concentration and colours a, b and L). As shown in this manuscript, ESPC tools allow for proper and systematic analysis of huge amounts of industrial data, using simple, fast and efficient statistical techniques, which can be used to improve the quality of the process operation in most industrial polymerisation plants. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21804" xmlns="http://purl.org/rss/1.0/"><title>Effect of small scale flow barriers heterogeneities and connate water on displacement efficiency of polymer floods to heavy oil reservoirs</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21804</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of small scale flow barriers heterogeneities and connate water on displacement efficiency of polymer floods to heavy oil reservoirs</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Saber Mohammadi, Mohammed Hossein Ghazanfari, Mohsen Masihi, Shapour Vossoughi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-18T09:50:53.291197-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21804</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21804</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21804</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena, Fluid Dynamics and Thermodynamics</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 concerns a fundamental understanding of how heterogeneities induced by flow barriers and connate water affect the displacement efficiency of polymer floods, which has rarely been studied in the available literature. Here, a series of water/polymer injection experiments to heavy oil performed on five-spot glass micromodels containing randomly distributed shale structures is presented. It has been found that macroscopic efficiency of polymer flooding majorly depends on flow barriers distribution/configuration; shale content and geometrical characteristics; presence of connate water and wettability of medium. Microscopic pictures revealed that the main parts of connate water were trapped in some pores/throats near and especially behind the shale streaks; also, presence of connate water causes a reduction of sweep efficiency due to premature breakthrough of displacing fluid in an oil-wet media. In absence of connate water, polymer solution could linger and stick to the pore walls to delay the time for a polymer to channel to the production site. Results of this work disclose requirements for a detailed geologic study of barrier size and distribution for successful design of EOR processes in heterogeneous reservoirs. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

This work concerns a fundamental understanding of how heterogeneities induced by flow barriers and connate water affect the displacement efficiency of polymer floods, which has rarely been studied in the available literature. Here, a series of water/polymer injection experiments to heavy oil performed on five-spot glass micromodels containing randomly distributed shale structures is presented. It has been found that macroscopic efficiency of polymer flooding majorly depends on flow barriers distribution/configuration; shale content and geometrical characteristics; presence of connate water and wettability of medium. Microscopic pictures revealed that the main parts of connate water were trapped in some pores/throats near and especially behind the shale streaks; also, presence of connate water causes a reduction of sweep efficiency due to premature breakthrough of displacing fluid in an oil-wet media. In absence of connate water, polymer solution could linger and stick to the pore walls to delay the time for a polymer to channel to the production site. Results of this work disclose requirements for a detailed geologic study of barrier size and distribution for successful design of EOR processes in heterogeneous reservoirs. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21773" xmlns="http://purl.org/rss/1.0/"><title>Simplified kinetic model for steam reforming of ethanol on a Ni/Al2O3 catalyst</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21773</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Simplified kinetic model for steam reforming of ethanol on a Ni/Al2O3 catalyst</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Y.-J. Wu, J.C. Santos, Ping Li, J.-G. Yu, A.F. Cunha, A.E. Rodrigues</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-18T09:50:48.722077-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21773</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21773</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21773</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, Chemical Kinetics and Catalysis</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>Ethanol steam reforming is a promising method for hydrogen production. Kinetic studies are carried out over a nickel-based catalyst from 200 to 600°C. A simplified Langmuir–Hinshelwood–Hougen–Watson (LHHW) kinetic model was proposed with nine parameters, where the surface decomposition of methane is assumed as the rate determining step (RDS), and while all other reaction steps are set as reversible. It is postulated that the velocity of the backward reaction step of the dissociative methane adsorption <span class="math"><img alt="equation image" src="http://onlinelibrary.wiley.com/store/10.1002/cjce.21773/asset/equation/tex2gif-ueqn-1.gif?v=1&amp;s=d948cfd3d348b498116a791947329d00f978cc9d" class="inlineGraphic"/></span> is similar to all other equilibrium reactions proposed, while the forward reaction step is set as the RDS. In addition, the formation of adsorbed carbon species is excluded due to the fact that SRE experiments were performed with excess water, suggesting that OH species, excluding O species formation, stick better on active Ni surface than methane. In addition, a power law kinetic model was used for analysis; the activation energy was 31.8 kJ/mol, and the reaction order of ethanol pressure was 1.52. Experimental results were successfully demonstrated by both kinetic models. The purpose of this work was to develop a simplified mechanistic model to replace empirical models (power rate model) and other proposed kinetic models that are too complex for an applied kinetic process. It was found that the simplified LHHW kinetic model has a better fit than that of the power law model. The proposed kinetic model works well over a wide temperature range (200–600°C). © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Ethanol steam reforming is a promising method for hydrogen production. Kinetic studies are carried out over a nickel-based catalyst from 200 to 600°C. A simplified Langmuir–Hinshelwood–Hougen–Watson (LHHW) kinetic model was proposed with nine parameters, where the surface decomposition of methane is assumed as the rate determining step (RDS), and while all other reaction steps are set as reversible. It is postulated that the velocity of the backward reaction step of the dissociative methane adsorption ${\rm CH}_4 + 2\left){\vphantom{1{}}}\right.\!\!\!\!\overline{\,\,\,\vphantom 1{{}}}\left){\vphantom{1{{\rm CH}_3 }}}\right.\!\!\!\!\overline{\,\,\,\vphantom 1{{{\rm CH}_3 }}} + \left){\vphantom{1{\rm H}}}\right.\!\!\!\!\overline{\,\,\,\vphantom 1{{\rm H}}}$ is similar to all other equilibrium reactions proposed, while the forward reaction step is set as the RDS. In addition, the formation of adsorbed carbon species is excluded due to the fact that SRE experiments were performed with excess water, suggesting that OH species, excluding O species formation, stick better on active Ni surface than methane. In addition, a power law kinetic model was used for analysis; the activation energy was 31.8 kJ/mol, and the reaction order of ethanol pressure was 1.52. Experimental results were successfully demonstrated by both kinetic models. The purpose of this work was to develop a simplified mechanistic model to replace empirical models (power rate model) and other proposed kinetic models that are too complex for an applied kinetic process. It was found that the simplified LHHW kinetic model has a better fit than that of the power law model. The proposed kinetic model works well over a wide temperature range (200–600°C). © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21821" xmlns="http://purl.org/rss/1.0/"><title>Spray characteristics of a swirl atomiser in trigger sprayers using water–ethanol mixtures</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21821</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Spray characteristics of a swirl atomiser in trigger sprayers using water–ethanol mixtures</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Shanshan Yao, Tiegang Fang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-18T09:50:48.309781-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21821</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21821</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21821</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena, Fluid Dynamics and Thermodynamics</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>Pressure swirl atomisers are widely used in both industry and daily life. It is critical to understand the spray transient behaviour for better design of these systems. This paper presents an experimental study of conical liquid sheets breakup from a swirl atomiser nozzle in trigger sprayers. Spray and atomisation characteristics were measured and analysed. Water–ethanol mixtures were used to simulate different fluids on the breakup and atomisation quality of the spray development process with a wide range of surface tension while maintaining relatively small changes in fluid viscosity and density. The spray images were taken by a high speed digital camera and post-processed to analyse the global spray structure, spray cone angle, and breakup length. The droplet size and its distribution were measured using a laser diffraction technique. It was observed that the surface waves grow rapidly on the cone-shaped liquid sheets and breakup into liquid ligaments and droplets during the initial stage of fluid dispensing. Then the spray transitions into the developed stage. Near the end of the dispensing process, the liquid cone collapses with poor atomisation (large droplets) due to momentum loss. The comparison between different fluids showed that the spray cone angle and liquid breakup length decreased with the increase of ethanol percentage ratio. The percentiles parameters, Sauter mean diameter (SMD) and particle size distribution were measured and compared for different locations. High surface tension fluids produce larger droplets than lower surface tension fluids, which have the same trend as the percentiles parameters and SMD. Results also show that droplet size and its distribution depend on the location of the measurement. Generally speaking, smaller droplet size is found for a location away from the nozzle axis in the vertical direction. In the horizontal direction, larger droplet sizes are found for a location closer to the nozzle exit. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Pressure swirl atomisers are widely used in both industry and daily life. It is critical to understand the spray transient behaviour for better design of these systems. This paper presents an experimental study of conical liquid sheets breakup from a swirl atomiser nozzle in trigger sprayers. Spray and atomisation characteristics were measured and analysed. Water–ethanol mixtures were used to simulate different fluids on the breakup and atomisation quality of the spray development process with a wide range of surface tension while maintaining relatively small changes in fluid viscosity and density. The spray images were taken by a high speed digital camera and post-processed to analyse the global spray structure, spray cone angle, and breakup length. The droplet size and its distribution were measured using a laser diffraction technique. It was observed that the surface waves grow rapidly on the cone-shaped liquid sheets and breakup into liquid ligaments and droplets during the initial stage of fluid dispensing. Then the spray transitions into the developed stage. Near the end of the dispensing process, the liquid cone collapses with poor atomisation (large droplets) due to momentum loss. The comparison between different fluids showed that the spray cone angle and liquid breakup length decreased with the increase of ethanol percentage ratio. The percentiles parameters, Sauter mean diameter (SMD) and particle size distribution were measured and compared for different locations. High surface tension fluids produce larger droplets than lower surface tension fluids, which have the same trend as the percentiles parameters and SMD. Results also show that droplet size and its distribution depend on the location of the measurement. Generally speaking, smaller droplet size is found for a location away from the nozzle axis in the vertical direction. In the horizontal direction, larger droplet sizes are found for a location closer to the nozzle exit. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21823" xmlns="http://purl.org/rss/1.0/"><title>Investigation on alternative disposal methods for froth treatment tailings—part 1, disposal without asphaltene recovery</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21823</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Investigation on alternative disposal methods for froth treatment tailings—part 1, disposal without asphaltene recovery</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yuming Xu, Tadek Dabros, Jianmin Kan</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-26T09:18:14.318747-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21823</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21823</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21823</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Special Issue Article on Oil Sands 2012</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 paraffinic froth treatment, tailings from the tailings solvent recovery unit (TSRU) contain a significant fraction of asphaltenes. In current commercial practice, the TSRU tailings are disposed of in a tailings pond where the large asphaltene particles and coarse tailings settle and the fines form mature fine tailings (MFT). With increasing public concern about the environmental impact of tailings ponds and stricter government regulations on tailings disposal, the oil sand industry has increased efforts to find alternatives that eliminate or reduce the use of tailings ponds. In collaboration with Total E&amp;P Canada (TEPCA), CanmetENERGY conducted an extensive research program to explore alternatives for TSRU tailings disposal. TSRU tailings were produced from TEPCA's froth treatment pilot tests conducted at the CanmetENERGY froth treatment facility. Various processes were investigated, including flocculation and thickening, filtration, and centrifugation. A large number of bench-scale flocculation-thickening and filtration tests were conducted, followed by numerous pilot-scale flocculation-thickening tests and centrifugation tests. The experimental results demonstrate that TSRU tailings can be flocculated and thickened to produce paste-like sediment, and the hot water can be recovered and recycled. The thickened TSRU tailings have good water drainage and deposition of the sediment on a beach would result in further dewatering. Centrifugation of the TSRU tailings or filtration of the thickener underflow can produce a cake that appears to be very dry and suitable for disposal without pond containment. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

In paraffinic froth treatment, tailings from the tailings solvent recovery unit (TSRU) contain a significant fraction of asphaltenes. In current commercial practice, the TSRU tailings are disposed of in a tailings pond where the large asphaltene particles and coarse tailings settle and the fines form mature fine tailings (MFT). With increasing public concern about the environmental impact of tailings ponds and stricter government regulations on tailings disposal, the oil sand industry has increased efforts to find alternatives that eliminate or reduce the use of tailings ponds. In collaboration with Total E&amp;P Canada (TEPCA), CanmetENERGY conducted an extensive research program to explore alternatives for TSRU tailings disposal. TSRU tailings were produced from TEPCA's froth treatment pilot tests conducted at the CanmetENERGY froth treatment facility. Various processes were investigated, including flocculation and thickening, filtration, and centrifugation. A large number of bench-scale flocculation-thickening and filtration tests were conducted, followed by numerous pilot-scale flocculation-thickening tests and centrifugation tests. The experimental results demonstrate that TSRU tailings can be flocculated and thickened to produce paste-like sediment, and the hot water can be recovered and recycled. The thickened TSRU tailings have good water drainage and deposition of the sediment on a beach would result in further dewatering. Centrifugation of the TSRU tailings or filtration of the thickener underflow can produce a cake that appears to be very dry and suitable for disposal without pond containment. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21812" xmlns="http://purl.org/rss/1.0/"><title>Turbulence effects on the granular model of particle motion in a boundary layer flow</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21812</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Turbulence effects on the granular model of particle motion in a boundary layer flow</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Maziar Dehghan, Hassan Basirat Tabrizi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-26T09:18:13.912129-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21812</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21812</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21812</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena, Fluid Dynamics and Thermodynamics</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>Prediction of particle velocity in a dilute turbulent gas–particle flow nearby a flat solid boundary is investigated numerically using a fully Eulerian two-fluid model. The particulate phase model is based on the kinetic theory of granular flow. The turbulence in both phases is modelled. Inter-particle and particle-wall inelastic collisions are considered. Effects of presence/absence of particulate phase turbulence modelling on velocity of particles are investigated. Results indicate that turbulence modelling is necessary for particulate phase, but conventional models should be modified to consider particulate flow nature. Effects of free stream velocity and particle diameter on turbulence modelling results have been discussed. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Prediction of particle velocity in a dilute turbulent gas–particle flow nearby a flat solid boundary is investigated numerically using a fully Eulerian two-fluid model. The particulate phase model is based on the kinetic theory of granular flow. The turbulence in both phases is modelled. Inter-particle and particle-wall inelastic collisions are considered. Effects of presence/absence of particulate phase turbulence modelling on velocity of particles are investigated. Results indicate that turbulence modelling is necessary for particulate phase, but conventional models should be modified to consider particulate flow nature. Effects of free stream velocity and particle diameter on turbulence modelling results have been discussed. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21814" xmlns="http://purl.org/rss/1.0/"><title>Removal of Cu2+ and Pb2+ ions by N-vinyl 2-pyrrolidone/itaconic acid hydrogels from aqueous solutions</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21814</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Removal of Cu2+ and Pb2+ ions by N-vinyl 2-pyrrolidone/itaconic acid hydrogels from aqueous solutions</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mümin Evren, Işıl Acar, Kubilay Güçlü, Gamze Güçlü</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-26T09:18:12.024765-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21814</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21814</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21814</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Environment, Renewable Resources and Green Processes</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 study, a series of crosslinked <em>N</em>-vinyl-2-pyrrolidone–itaconic acid (NVP-IA) hydrogels was prepared by free radical polymerisation in aqueous solution. Swelling, mechanical and adsorption properties for the removal of Cu<sup>2+</sup> and Pb<sup>2+</sup> ions from aqueous solutions of these hydrogels were investigated. Metal ion adsorption capacities of hydrogels for Cu<sup>2+</sup> and Pb<sup>2+</sup> ions were determined as 2.1 and 0.6 mmol g<sup>−1</sup>, respectively. Adsorption processes of metal ions onto the NVP-IA hydrogels follow pseudo-second-order type adsorption kinetics. The equilibrium adsorption data have been evaluated using Freundlich and Langmuir isotherm models. The results illustrated that the adsorption follows Freundlich isotherm. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

In this study, a series of crosslinked N-vinyl-2-pyrrolidone–itaconic acid (NVP-IA) hydrogels was prepared by free radical polymerisation in aqueous solution. Swelling, mechanical and adsorption properties for the removal of Cu2+ and Pb2+ ions from aqueous solutions of these hydrogels were investigated. Metal ion adsorption capacities of hydrogels for Cu2+ and Pb2+ ions were determined as 2.1 and 0.6 mmol g−1, respectively. Adsorption processes of metal ions onto the NVP-IA hydrogels follow pseudo-second-order type adsorption kinetics. The equilibrium adsorption data have been evaluated using Freundlich and Langmuir isotherm models. The results illustrated that the adsorption follows Freundlich isotherm. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21815" xmlns="http://purl.org/rss/1.0/"><title>Process optimisation of porous carbon preparation from date palm Pits and adsorption kinetics of methylene blue</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21815</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Process optimisation of porous carbon preparation from date palm Pits and adsorption kinetics of methylene blue</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Kashif Rashid, K. Suresh Kumar Reddy, Ahmed Al Shoaibi, C. Srinivasakannan</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-26T09:18:10.769565-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21815</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21815</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21815</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Environment, Renewable Resources and Green Processes</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 present study focuses on the process optimisation of porous carbon preparation from date seed pits. The response surface methodology (RSM) technique with Box–Behnken method (BBM) was utilised with the response variables being the yield and BET surface area. The influencing parameters selected were activation temperature, impregnation ratio (IR) and activation time. The optimum conditions were identified to be an activation temperature of 500°C, IR of 2 and activation time of 75 min, with the resulting yield and BET surface area being 46% and 838 m<sup>2</sup>/g. The average pore volume and average pore diameter were 1.07 cm<sup>3</sup>/g and 1.69 nm, respectively. In order to assess the suitability of the carbon for adsorption of macromolecules, the kinetics of methylene blue (MB) adsorption were assessed by varying the initial concentration and the adsorption temperature. The kinetic parameters were evaluated applying the pseudo-second-order kinetic model by minimising the error between the experimental data and the model prediction; it was found to represent the experimental data more aptly. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

The present study focuses on the process optimisation of porous carbon preparation from date seed pits. The response surface methodology (RSM) technique with Box–Behnken method (BBM) was utilised with the response variables being the yield and BET surface area. The influencing parameters selected were activation temperature, impregnation ratio (IR) and activation time. The optimum conditions were identified to be an activation temperature of 500°C, IR of 2 and activation time of 75 min, with the resulting yield and BET surface area being 46% and 838 m2/g. The average pore volume and average pore diameter were 1.07 cm3/g and 1.69 nm, respectively. In order to assess the suitability of the carbon for adsorption of macromolecules, the kinetics of methylene blue (MB) adsorption were assessed by varying the initial concentration and the adsorption temperature. The kinetic parameters were evaluated applying the pseudo-second-order kinetic model by minimising the error between the experimental data and the model prediction; it was found to represent the experimental data more aptly. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21816" xmlns="http://purl.org/rss/1.0/"><title>Removal of mercaptans from gas–oil using synthesised anatase form of TiO2 nanoparticles</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21816</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Removal of mercaptans from gas–oil using synthesised anatase form of TiO2 nanoparticles</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mehdi Karimi, Fakhry Seyedeyn-Azad, Jalal Abedi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-26T09:18:08.230283-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21816</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21816</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21816</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Environment, Renewable Resources and Green Processes</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>High purity titanium dioxide (TiO<sub>2</sub>) nanoparticles were synthesised via a modified sol–gel method using titanium tetraisopropoxide (TTIP). XRD analysis showed that the synthesised product was TiO<sub>2</sub> powder in anatase form. The sample possessed a relatively high surface area of 75.64 m<sup>2</sup>/g. The typical TEM images suggested that the crystalline phase product was composed of fine particles with dimensions between 17 and 20 nm. The synthesised material was used as a photocatalyst for the removal of mercaptans from gas–oil. The result showed that up to 78% of the mercaptans in gas–oil was removed using the synthesised TiO<sub>2</sub> photocatalyst. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

High purity titanium dioxide (TiO2) nanoparticles were synthesised via a modified sol–gel method using titanium tetraisopropoxide (TTIP). XRD analysis showed that the synthesised product was TiO2 powder in anatase form. The sample possessed a relatively high surface area of 75.64 m2/g. The typical TEM images suggested that the crystalline phase product was composed of fine particles with dimensions between 17 and 20 nm. The synthesised material was used as a photocatalyst for the removal of mercaptans from gas–oil. The result showed that up to 78% of the mercaptans in gas–oil was removed using the synthesised TiO2 photocatalyst. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21810" xmlns="http://purl.org/rss/1.0/"><title>Study on the flow structure and its effects on the interaction and formation of cryogenic Taylor bubbles By PIV technique and POD analysis</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21810</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Study on the flow structure and its effects on the interaction and formation of cryogenic Taylor bubbles By PIV technique and POD analysis</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yi-Peng Liu, Ping-Yang Wang, Xian-Lin Zhao, Zhao-Hui Du</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-26T09:18:06.496489-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21810</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21810</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21810</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena, Fluid Dynamics and Thermodynamics</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 flow structures around continuous cryogenic Taylor bubbles in the concentric glass tube with different diameters were investigated using particle image velocimetry (PIV) technique under various inclination angles. Optical distortions produced by tube curvature and the refractive index differences between tube and fluid were corrected using ray tracing method. Based on the PIV results, the proper orthogonal decomposition (POD) method was used to investigate the effect of flow structure on the interaction of Taylor bubbles through the large-scale turbulent structures of POD modes. Four best-fitted curves for Taylor bubble interaction for different inclination angles were represented. A correlation for Taylor bubble formation was developed with the consideration of turbulence suppression, tube inner diameter, fluid properties, inclination angle, etc. The results demonstrate that the minimum stable distance attains the smallest value at <em>θ</em> = 60°. The correlation for Taylor bubble formation shows good agreement with the experimental data both in the present study and from its references. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

The flow structures around continuous cryogenic Taylor bubbles in the concentric glass tube with different diameters were investigated using particle image velocimetry (PIV) technique under various inclination angles. Optical distortions produced by tube curvature and the refractive index differences between tube and fluid were corrected using ray tracing method. Based on the PIV results, the proper orthogonal decomposition (POD) method was used to investigate the effect of flow structure on the interaction of Taylor bubbles through the large-scale turbulent structures of POD modes. Four best-fitted curves for Taylor bubble interaction for different inclination angles were represented. A correlation for Taylor bubble formation was developed with the consideration of turbulence suppression, tube inner diameter, fluid properties, inclination angle, etc. The results demonstrate that the minimum stable distance attains the smallest value at θ = 60°. The correlation for Taylor bubble formation shows good agreement with the experimental data both in the present study and from its references. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21809" xmlns="http://purl.org/rss/1.0/"><title>Thermodiffusion effect for a non-associating mixture in a multi layered system of porous media and fluid layers heated from above</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21809</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Thermodiffusion effect for a non-associating mixture in a multi layered system of porous media and fluid layers heated from above</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">H. Jawad, H. Bataller, M.Z. Saghir</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-26T09:17:59.686508-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21809</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21809</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21809</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena, Fluid Dynamics and Thermodynamics</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 numerical simulation has been conducted to investigate the thermodiffusion phenomenon in a porous layer sandwiched between two liquid layers that are wetted with water alcohol mixtures at different water concentrations. Two different binary mixtures with different Soret coefficients have been used in the entire system, one with a negative Soret coefficient and the other one with a positive sign. The results show that the direction of the component migration in a porous layer depends on the sign of the Soret coefficient. For a binary mixture with a negative Soret coefficient, such as 10% isopropanol and 90% water, the heavier species move in the direction of the hot surface, while for a mixture with a positive Soret effect, such as 50% isopropanol and 50% water, the heavier species migrate toward the colder surface. To reduce the gravity effect, the cavity was heated from the top with different temperatures ranging from 5 to 20 K. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

A numerical simulation has been conducted to investigate the thermodiffusion phenomenon in a porous layer sandwiched between two liquid layers that are wetted with water alcohol mixtures at different water concentrations. Two different binary mixtures with different Soret coefficients have been used in the entire system, one with a negative Soret coefficient and the other one with a positive sign. The results show that the direction of the component migration in a porous layer depends on the sign of the Soret coefficient. For a binary mixture with a negative Soret coefficient, such as 10% isopropanol and 90% water, the heavier species move in the direction of the hot surface, while for a mixture with a positive Soret effect, such as 50% isopropanol and 50% water, the heavier species migrate toward the colder surface. To reduce the gravity effect, the cavity was heated from the top with different temperatures ranging from 5 to 20 K. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21806" xmlns="http://purl.org/rss/1.0/"><title>Experimental study on adsorption of a new surfactant onto carbonate reservoir samples—application to EOR</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21806</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Experimental study on adsorption of a new surfactant onto carbonate reservoir samples—application to EOR</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sohrab Zendehboudi, Mohammad Ali Ahmadi, Amin Reza Rajabzadeh, Nader Mahinpey, Ioannis Chatzis</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-18T07:41:04.503198-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21806</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21806</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21806</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Interfacial and Electrochemical Phenomena</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>Surfactant flooding aims at lowering the interfacial tensions between the oil and water phases to improve the displacement efficiency during oil recovery. However, surfactant losses due to adsorption on the reservoir rock impairs performance of the chemical flooding, consequently renders the process impractical economically. This article presents adsorption equilibrium and kinetics of Zizyphus Spina Christi (ZSC), a new non-ionic surfactant, onto carbonate rocks. The adsorption tests were conducted at a temperature range of 28–75°C. A conductivity method was employed in this study to measure CMC parameter and surfactant concentration in the aqueous solutions. The equilibrium conditions for the crushed rock samples were obtained after about 2 days. According to the experimental results, the equilibrium data were well-fitted by the Freundlich isotherm for carbonate samples. Furthermore, the adsorption process is exothermic and obeys the second-order kinetic model. Such a systematic investigation is very helpful to select a proper surfactant for EOR application and reservoir stimulation in the petroleum industry. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Surfactant flooding aims at lowering the interfacial tensions between the oil and water phases to improve the displacement efficiency during oil recovery. However, surfactant losses due to adsorption on the reservoir rock impairs performance of the chemical flooding, consequently renders the process impractical economically. This article presents adsorption equilibrium and kinetics of Zizyphus Spina Christi (ZSC), a new non-ionic surfactant, onto carbonate rocks. The adsorption tests were conducted at a temperature range of 28–75°C. A conductivity method was employed in this study to measure CMC parameter and surfactant concentration in the aqueous solutions. The equilibrium conditions for the crushed rock samples were obtained after about 2 days. According to the experimental results, the equilibrium data were well-fitted by the Freundlich isotherm for carbonate samples. Furthermore, the adsorption process is exothermic and obeys the second-order kinetic model. Such a systematic investigation is very helpful to select a proper surfactant for EOR application and reservoir stimulation in the petroleum industry. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21811" xmlns="http://purl.org/rss/1.0/"><title>Numerical study of counter-current gas–solid flow in FCC disengager and stripper</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21811</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Numerical study of counter-current gas–solid flow in FCC disengager and stripper</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dening Jia, Hui Zhao, Abdallah S. Berrouk, Chaohe Yang, Honghong Shan</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-18T07:41:01.759934-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21811</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21811</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21811</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena, Fluid Dynamics and Thermodynamics</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>Detailed study of the gas–solid flow in FCC reactor was performed using Euler–Euler two-fluid model. Two distinct regions were identified in the reactor vessel based on differences in catalyst void fraction and fluid flow: the dilute phase congested disengager region and dense phase congested stripper region. Velocity profile revealed an inert yet random flow pattern in the disengager and a counter-current type of flow with a pronounced radial unevenness in the stripper. Residence time distribution proved that a small portion of oil vapour could linger over 5 min before exiting despite that the apparatus may have a significantly shorter average residence time. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Detailed study of the gas–solid flow in FCC reactor was performed using Euler–Euler two-fluid model. Two distinct regions were identified in the reactor vessel based on differences in catalyst void fraction and fluid flow: the dilute phase congested disengager region and dense phase congested stripper region. Velocity profile revealed an inert yet random flow pattern in the disengager and a counter-current type of flow with a pronounced radial unevenness in the stripper. Residence time distribution proved that a small portion of oil vapour could linger over 5 min before exiting despite that the apparatus may have a significantly shorter average residence time. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21771" xmlns="http://purl.org/rss/1.0/"><title>An overview of conversion of residues from coal liquefaction processes</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21771</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">An overview of conversion of residues from coal liquefaction processes</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Khare, M. Dell'Amico</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-18T07:41:00.273411-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21771</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21771</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21771</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Process Systems Engineering</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>Direct coal liquefaction (DCL) is a process for converting coal to synthetic oils, which can be refined to make transportation fuels. Residue from this process contains inorganic material such as mineral matter originating from the coal and catalysts, and organic matter such as unconverted coal, heavy oils, pre-asphaltenes and asphaltenes. The conversion of these DCL residues to lighter, high-value products is an important step in helping to make this technology both commercially viable and environmentally acceptable. This paper provides an overview of the physico-chemical characteristics and processing options available for coal liquefaction residues and compares and contrasts them to those of petroleum residues.</p></div>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Residue properties vary considerably, since they are highly dependent on feed coal, process configuration and operating conditions. Determination of composition and structural parameters of products derived from residue conversion can help determine their stability, coking and solvent hydrogen donating ability. Thermal conversion processes such as visbreaking and gasification offer the greatest promise for handling these heavy materials. The conversion chemistry, reactivity and kinetics of residue gasification are not well-understood but are important in optimising hydrogen production for the process.</p></div>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The literature has been comprehensively reviewed to provide characteristics and properties of residues and their potential for conversion. In addition, the potential for producing high-value carbon products from residues is briefly discussed. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Direct coal liquefaction (DCL) is a process for converting coal to synthetic oils, which can be refined to make transportation fuels. Residue from this process contains inorganic material such as mineral matter originating from the coal and catalysts, and organic matter such as unconverted coal, heavy oils, pre-asphaltenes and asphaltenes. The conversion of these DCL residues to lighter, high-value products is an important step in helping to make this technology both commercially viable and environmentally acceptable. This paper provides an overview of the physico-chemical characteristics and processing options available for coal liquefaction residues and compares and contrasts them to those of petroleum residues.
Residue properties vary considerably, since they are highly dependent on feed coal, process configuration and operating conditions. Determination of composition and structural parameters of products derived from residue conversion can help determine their stability, coking and solvent hydrogen donating ability. Thermal conversion processes such as visbreaking and gasification offer the greatest promise for handling these heavy materials. The conversion chemistry, reactivity and kinetics of residue gasification are not well-understood but are important in optimising hydrogen production for the process.
The literature has been comprehensively reviewed to provide characteristics and properties of residues and their potential for conversion. In addition, the potential for producing high-value carbon products from residues is briefly discussed. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21799" xmlns="http://purl.org/rss/1.0/"><title>Ultrasound-assisted adsorption of reactive blue 21 dye on TiO2 in the presence of some rare earths (La, Ce, Pr &amp; Gd)</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21799</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Ultrasound-assisted adsorption of reactive blue 21 dye on TiO2 in the presence of some rare earths (La, Ce, Pr &amp; Gd)</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Pankaj Srivastava, Shikha Goyal, Rajesh Tayade</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-18T07:40:59.881032-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21799</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21799</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21799</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Environment, Renewable Resources and Green Processes</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>Adsorption of reactive blue (RB) 21 dye in the aqueous solution has been carried out on TiO<sub>2</sub> alone and in combination with rare earth ions [La<sup>3+</sup>, Ce<sup>4+</sup>, Pr<sup>3+</sup> and Gd<sup>3+</sup>] in the presence and absence of ultrasound. The formation of adsorbent (TiO<sub>2</sub>) from tetra <em>n</em>-butyl orthotitanate and its characterisation has been done through X-ray diffraction (XRD), scanning electron microscopy (SEM), diffuse reflectance spectroscopy (DRS), Raman spectroscopy and N<sub>2</sub> adsorption techniques. Complete decolourisation was achieved in 5 min in the presence of US + TiO<sub>2</sub> + Ce. The effects of initial concentration of dye, adsorbent dose and contact time on the decolourisation of dye have been examined under different experimental conditions. The removal of dye in the presence of ultrasound was (88–99%) compared to conventional stirring (62–69%).</p></div>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Adsorption behaviour has been analysed using Langmuir, Freundlich, Dubinin–Radushkevich and Temkin isotherm models. RE–TiO<sub>2</sub> combination had higher adsorption equilibrium constant (<em>K</em><sub>c</sub>) and better adsorption capacity (<em>q</em><sub>max</sub>) than TiO<sub>2</sub> alone, both in the absence and presence of ultrasound, indicating the formation of Dye-RE complex before sorption. This is confirmed from the shift in <em>λ</em><sub>max</sub> from 626 to 616 cm<sup>−1</sup>. The kinetic data fit well with the pseudo-second order kinetic model, and the adsorption process was spontaneous in the presence of rare earths. The mechanism of adsorption has been explained with the help of Weber–Morris intraparticle diffusion and Boyd kinetic models. A batch adsorber has been proposed for different TiO<sub>2</sub> dose to effluent volume ratios using the Langmuir equation. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Adsorption of reactive blue (RB) 21 dye in the aqueous solution has been carried out on TiO2 alone and in combination with rare earth ions [La3+, Ce4+, Pr3+ and Gd3+] in the presence and absence of ultrasound. The formation of adsorbent (TiO2) from tetra n-butyl orthotitanate and its characterisation has been done through X-ray diffraction (XRD), scanning electron microscopy (SEM), diffuse reflectance spectroscopy (DRS), Raman spectroscopy and N2 adsorption techniques. Complete decolourisation was achieved in 5 min in the presence of US + TiO2 + Ce. The effects of initial concentration of dye, adsorbent dose and contact time on the decolourisation of dye have been examined under different experimental conditions. The removal of dye in the presence of ultrasound was (88–99%) compared to conventional stirring (62–69%).
Adsorption behaviour has been analysed using Langmuir, Freundlich, Dubinin–Radushkevich and Temkin isotherm models. RE–TiO2 combination had higher adsorption equilibrium constant (Kc) and better adsorption capacity (qmax) than TiO2 alone, both in the absence and presence of ultrasound, indicating the formation of Dye-RE complex before sorption. This is confirmed from the shift in λmax from 626 to 616 cm−1. The kinetic data fit well with the pseudo-second order kinetic model, and the adsorption process was spontaneous in the presence of rare earths. The mechanism of adsorption has been explained with the help of Weber–Morris intraparticle diffusion and Boyd kinetic models. A batch adsorber has been proposed for different TiO2 dose to effluent volume ratios using the Langmuir equation. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21800" xmlns="http://purl.org/rss/1.0/"><title>Role of carrier flotation in accelerating bitumen extraction recovery from Mineable Athabasca oil sands</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21800</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Role of carrier flotation in accelerating bitumen extraction recovery from Mineable Athabasca oil sands</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Z.A. (Joe) Zhou, Haihong Li, Ross Chow, Kelly Roberge</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-18T07:40:59.536781-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21800</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21800</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21800</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Special issue: Oil Sands 2012</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>Ore blending is a strategy developed in the oil sands industry to enhance bitumen recovery from low grade oil sands ores. It involves blending low grade ores with high grade ores at a certain ratio, resulting in a higher overall bitumen recovery from the mixture than the simple recovery summation of the two extracted separately. To understand the underlying mechanisms, both bitumen-coated glass beads (−150 + 125 µm) and raw coal particles (−500 + 300, −300 + 150 and −150 µm) were used as carrier materials in this study to simulate bitumen droplets from high grade ores. Experimental results revealed that coal particles were more efficient than hydrophobised bitumen-coated glass beads in accelerating bitumen recovery and that better bitumen extraction performance was obtained by using smaller sizes of coal. This was attributed to the gravitational effect of larger, heavier particles on the detachment of bitumen-particle aggregates from bubbles. For smaller sizes of coal (−150 µm), a faster bitumen flotation recovery was achieved with more coal added. An increase in bitumen recovery up to 20–30% (absolute) was obtained by adding coal into the oil sands slurry. The interaction of bitumen with coal particles or bitumen-coated glass beads during oil sands slurry conditioning and flotation was visually verified from simple coagulation tests. The similarity of ore blending in oil sands extraction to carrier flotation in minerals flotation and the potential application of carrier flotation principles to oil sands extraction were discussed. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Ore blending is a strategy developed in the oil sands industry to enhance bitumen recovery from low grade oil sands ores. It involves blending low grade ores with high grade ores at a certain ratio, resulting in a higher overall bitumen recovery from the mixture than the simple recovery summation of the two extracted separately. To understand the underlying mechanisms, both bitumen-coated glass beads (−150 + 125 µm) and raw coal particles (−500 + 300, −300 + 150 and −150 µm) were used as carrier materials in this study to simulate bitumen droplets from high grade ores. Experimental results revealed that coal particles were more efficient than hydrophobised bitumen-coated glass beads in accelerating bitumen recovery and that better bitumen extraction performance was obtained by using smaller sizes of coal. This was attributed to the gravitational effect of larger, heavier particles on the detachment of bitumen-particle aggregates from bubbles. For smaller sizes of coal (−150 µm), a faster bitumen flotation recovery was achieved with more coal added. An increase in bitumen recovery up to 20–30% (absolute) was obtained by adding coal into the oil sands slurry. The interaction of bitumen with coal particles or bitumen-coated glass beads during oil sands slurry conditioning and flotation was visually verified from simple coagulation tests. The similarity of ore blending in oil sands extraction to carrier flotation in minerals flotation and the potential application of carrier flotation principles to oil sands extraction were discussed. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21801" xmlns="http://purl.org/rss/1.0/"><title>Double diffusive convection and thermodiffusion of fullerene–toluene nanofluid in a porous cavity</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21801</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Double diffusive convection and thermodiffusion of fullerene–toluene nanofluid in a porous cavity</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Amirhossein Ahadi, Tooraj Yousefi, M. Ziad Saghir</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-18T07:40:56.453636-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21801</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21801</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21801</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">New Materials, Nanomaterials and Nanotechnology Engineering</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 full Brinkman equation coupled with the heat and mass transfer equations was solved numerically using the finite element technique. A square cavity filled with hydrocarbon nanofluid of fullerene–toluene with different concentration values of fullerene was subject to various heating conditions. Results have confirmed that in the presence of nanofluid a heat transfer enhancement is present until a certain amount of initial concentration of the nanofluids. The heat convection coefficient was found to be 16% higher when nanofluid is used as the wetting fluid. In addition, it was determined that the concentration of fullerene in toluene has its limitation in heat removal enhancement. In fact, beyond 5% of fullerene, there is no noticeable enhancement of the heat removal in the system. The model was also used to study thermodiffusion effects in the cavity. Despite the small value and negligible effects of thermodiffusion in general heat and mass transfer problems, which is &lt;5% in the case of studying nanofluids, a maximum value of 20% variation of fullerene concentration has been detected. Moreover, fullerene separation was investigated for different heating intensities. As the Rayleigh number increases, the mixing was found to reduce the separation, which diminishes the Soret effect in the system. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

The full Brinkman equation coupled with the heat and mass transfer equations was solved numerically using the finite element technique. A square cavity filled with hydrocarbon nanofluid of fullerene–toluene with different concentration values of fullerene was subject to various heating conditions. Results have confirmed that in the presence of nanofluid a heat transfer enhancement is present until a certain amount of initial concentration of the nanofluids. The heat convection coefficient was found to be 16% higher when nanofluid is used as the wetting fluid. In addition, it was determined that the concentration of fullerene in toluene has its limitation in heat removal enhancement. In fact, beyond 5% of fullerene, there is no noticeable enhancement of the heat removal in the system. The model was also used to study thermodiffusion effects in the cavity. Despite the small value and negligible effects of thermodiffusion in general heat and mass transfer problems, which is &lt;5% in the case of studying nanofluids, a maximum value of 20% variation of fullerene concentration has been detected. Moreover, fullerene separation was investigated for different heating intensities. As the Rayleigh number increases, the mixing was found to reduce the separation, which diminishes the Soret effect in the system. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21802" xmlns="http://purl.org/rss/1.0/"><title>A developed smart technique to predict minimum miscible pressure—eor implications</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21802</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A developed smart technique to predict minimum miscible pressure—eor implications</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sohrab Zendehboudi, Mohammad Ali Ahmadi, Alireza Bahadori, Ali Shafiei, Tayfun Babadagli</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-18T07:40:53.369054-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21802</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21802</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21802</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena, Fluid Dynamics and Thermodynamics</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>Miscible gas injection (MGI) processes such as miscible CO<sub>2</sub> flooding have been in use as attractive EOR options, especially in conventional oil reserves. Optimal design of MGI is strongly dependent on parameters such as gas–oil minimum miscibility pressure (MMP), which is normally determined through expensive and time-consuming laboratory tests. Thus, developing a fast and reliable technique to predict gas–oil MMP is inevitable. To address this issue, a smart model is developed in this paper to forecast gas–oil MMP on the basis of a feed-forward artificial neural network (FF-ANN) combined with particle swarm optimisation (PSO). The MMP of a reservoir fluid was considered as a function of reservoir temperature and the compositions of oil and injected gas in the proposed model. Results of this study indicate that reservoir temperature among the input parameters selected for the PSO–ANN has the greatest impact on MMP value. The developed PSO–ANN model was examined using experimental data, and a reasonable match was attained showing a good potential for the proposed predictive tools in estimation of gas–oil MMP. Compared with other available methods, the proposed model is capable of forecasting oil–gas MMP more accurately in wide ranges of thermodynamic and process conditions. All predictive models used other than the PSO–ANN model failed in providing a good estimate of the oil–gas MMP of the hydrocarbon mixtures in Azadegan oilfield, Iran. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Miscible gas injection (MGI) processes such as miscible CO2 flooding have been in use as attractive EOR options, especially in conventional oil reserves. Optimal design of MGI is strongly dependent on parameters such as gas–oil minimum miscibility pressure (MMP), which is normally determined through expensive and time-consuming laboratory tests. Thus, developing a fast and reliable technique to predict gas–oil MMP is inevitable. To address this issue, a smart model is developed in this paper to forecast gas–oil MMP on the basis of a feed-forward artificial neural network (FF-ANN) combined with particle swarm optimisation (PSO). The MMP of a reservoir fluid was considered as a function of reservoir temperature and the compositions of oil and injected gas in the proposed model. Results of this study indicate that reservoir temperature among the input parameters selected for the PSO–ANN has the greatest impact on MMP value. The developed PSO–ANN model was examined using experimental data, and a reasonable match was attained showing a good potential for the proposed predictive tools in estimation of gas–oil MMP. Compared with other available methods, the proposed model is capable of forecasting oil–gas MMP more accurately in wide ranges of thermodynamic and process conditions. All predictive models used other than the PSO–ANN model failed in providing a good estimate of the oil–gas MMP of the hydrocarbon mixtures in Azadegan oilfield, Iran. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21797" xmlns="http://purl.org/rss/1.0/"><title>The relative exergy-destroyed array: A new tool for control structure design</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21797</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">The relative exergy-destroyed array: A new tool for control structure design</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M.T. Munir, W. Yu, B.R. Young</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-26T08:36:39.696181-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21797</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21797</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21797</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Process Control, Systems Engineering and Statistics</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>Due to increasing energy demands, energy crises and strict environmental regulations, the eco-efficiency of all industrial processes and plants has become vitally important. Control loop configuration or control system structure determination is a major and vitally important activity in the complex task of process control because a poorly structured control strategy can lose much energy from the process or plant when implemented. To save this loss of energy due to a poorly structured control strategy, engineers need to find a way to integrate control loop configuration and measurements of eco-efficiency. In this paper, we present the relative exergy-destroyed array (REDA), a new tool to measure the relative eco-efficiency of a process. The REDA is a means to compare the eco-efficiency of multi-input multi-output processes for different combinations of control structures. Based on steady state information, it is a simple tool for comparing eco-efficiency. The results obtained from the REDA are interpreted and explained with the help of case studies involving a whole monochlorobenzene (MCB) plant and a heat exchanger network (HEN). The REDA may help guide the process designer to quickly find a control design with low operating costs and high eco-efficiency. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Due to increasing energy demands, energy crises and strict environmental regulations, the eco-efficiency of all industrial processes and plants has become vitally important. Control loop configuration or control system structure determination is a major and vitally important activity in the complex task of process control because a poorly structured control strategy can lose much energy from the process or plant when implemented. To save this loss of energy due to a poorly structured control strategy, engineers need to find a way to integrate control loop configuration and measurements of eco-efficiency. In this paper, we present the relative exergy-destroyed array (REDA), a new tool to measure the relative eco-efficiency of a process. The REDA is a means to compare the eco-efficiency of multi-input multi-output processes for different combinations of control structures. Based on steady state information, it is a simple tool for comparing eco-efficiency. The results obtained from the REDA are interpreted and explained with the help of case studies involving a whole monochlorobenzene (MCB) plant and a heat exchanger network (HEN). The REDA may help guide the process designer to quickly find a control design with low operating costs and high eco-efficiency. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21794" xmlns="http://purl.org/rss/1.0/"><title>A new study on removal of cadmium by hybrid emulsion liquid membrane</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21794</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A new study on removal of cadmium by hybrid emulsion liquid membrane</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hamid Reza Mortaheb, Hossein Khormaei, Mohammad Hasan Amini, Babak Moktarani</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-26T08:36:35.976843-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21794</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21794</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21794</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separation Processes</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 application of hybrid emulsion liquid membrane, in which an O/W emulsion phase is placed between two supporting membranes, is applied in the present research for removal of cadmium from aqueous phase. The new setting has advantages such as higher stability of the emulsion phase, lower pollution of feed and stripping phases due to contacting with the membrane phase and higher removal capacity. Trioctylamine has been used as a carrier in the organic phase of the emulsion, while the applied surfactant is nonyl phenol ethoxylate. The effect of different parameters is investigated, such as pHs of aqueous and dispersed phases, organic to aqueous volume ratio in the emulsion, carrier concentration, temperature, stirring intensity and cadmium concentration in the feed phase on the performance of the system. The appropriate values of pH for stripping phase and the emulsion's aqueous phase are found to be about 13 and 7, respectively. The optimum organic to aqueous phase volume ratio in emulsion is found to be about 1. The removal efficiency increases approximately twice when the emulsion is stirred more rigorously. Applying the new setup can enhance the removal capacity comparing to the ultimate capacity obtained from the hybrid liquid membrane system. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

A new application of hybrid emulsion liquid membrane, in which an O/W emulsion phase is placed between two supporting membranes, is applied in the present research for removal of cadmium from aqueous phase. The new setting has advantages such as higher stability of the emulsion phase, lower pollution of feed and stripping phases due to contacting with the membrane phase and higher removal capacity. Trioctylamine has been used as a carrier in the organic phase of the emulsion, while the applied surfactant is nonyl phenol ethoxylate. The effect of different parameters is investigated, such as pHs of aqueous and dispersed phases, organic to aqueous volume ratio in the emulsion, carrier concentration, temperature, stirring intensity and cadmium concentration in the feed phase on the performance of the system. The appropriate values of pH for stripping phase and the emulsion's aqueous phase are found to be about 13 and 7, respectively. The optimum organic to aqueous phase volume ratio in emulsion is found to be about 1. The removal efficiency increases approximately twice when the emulsion is stirred more rigorously. Applying the new setup can enhance the removal capacity comparing to the ultimate capacity obtained from the hybrid liquid membrane system. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21765" xmlns="http://purl.org/rss/1.0/"><title>Simulation of pellet model with multicomponent mass diffusion closure using least squares spectral element solution method</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21765</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Simulation of pellet model with multicomponent mass diffusion closure using least squares spectral element solution method</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">K. R. Rout, H. A. Jakobsen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-05T08:20:29.644243-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21765</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21765</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21765</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, Chemical Kinetics and Catalysis</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>Mass- and mole-based pellet models have been solved using least-squares formulation to describe the evolution of species composition, pressure, velocity, total concentration and mass diffusion fluxes in porous pellets for the steam methane reforming (SMR) process. The objective of this work has been to compare the mass- and mole-based diffusion flux models, convection and fluid velocity for the SMR process using the least-squares spectral element method (LS-SEM). The diffusion–reaction problems are computationally intensive, requiring efficient numerical methods for dealing with them. This paper presents formulation and algorithm of LS-SEM for solving multicomponent mass diffusion pellet models. The mass diffusion flux is described according to the rigorous Maxwell Stefan model. This flux may be defined either with molar- or mass-averaged velocities. The effectiveness factors have been calculated for the SMR process and compared with the literature data.</p></div>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The model evaluations revealed that:
</p><ul id="l1" class="bullet">
<li>
<div class="para"><p>The least-squares method is well-suited for solving the multicomponent mass diffusion pellet models for the SMR process, achieving exponential convergence.</p></div>
</li>
<li>
<div class="para"><p>Molar- and mass-based pellet models do not give fully identical results for the SMR process, since the pellet model is not completely consistent.</p></div>
</li>
</ul><p> © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Mass- and mole-based pellet models have been solved using least-squares formulation to describe the evolution of species composition, pressure, velocity, total concentration and mass diffusion fluxes in porous pellets for the steam methane reforming (SMR) process. The objective of this work has been to compare the mass- and mole-based diffusion flux models, convection and fluid velocity for the SMR process using the least-squares spectral element method (LS-SEM). The diffusion–reaction problems are computationally intensive, requiring efficient numerical methods for dealing with them. This paper presents formulation and algorithm of LS-SEM for solving multicomponent mass diffusion pellet models. The mass diffusion flux is described according to the rigorous Maxwell Stefan model. This flux may be defined either with molar- or mass-averaged velocities. The effectiveness factors have been calculated for the SMR process and compared with the literature data.
The model evaluations revealed that:


The least-squares method is well-suited for solving the multicomponent mass diffusion pellet models for the SMR process, achieving exponential convergence.


Molar- and mass-based pellet models do not give fully identical results for the SMR process, since the pellet model is not completely consistent.

 © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21760" xmlns="http://purl.org/rss/1.0/"><title>Dehydration of methanol to dimethyl ether over γ-Al2O3 catalyst: Intrinsic kinetics and effectiveness factor</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21760</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Dehydration of methanol to dimethyl ether over γ-Al2O3 catalyst: Intrinsic kinetics and effectiveness factor</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Liang Zhang, Haitao Zhang, Weiyong Ying, Dingye Fang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-05T08:20:28.632104-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21760</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21760</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21760</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<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>Dehydration of methanol to dimethyl ether (DME) over a commercial γ-Al<sub>2</sub>O<sub>3</sub> catalyst was studied at the temperature interval 513–613 K, liquid hourly space velocity (LHSV) of 0.9–6.0 h<sup>−1</sup> and pressures between 0.1 and 1.0 MPa. The effect of different operation conditions on the dehydration of methanol was investigated in an isothermal fixed bed reactor. A kinetic equation which describes a Langmuir–Hinshelwood surface controlled reaction with dissociative adsorption of methanol was found to fit the experimental results quite well. An activation energy of 62.4 kJ/mol was obtained for the catalyst. A two-dimensional reaction–diffusion model was established for a cylindrical-shaped methanol dehydration catalyst. The internal effectiveness factor and the concentration distribution of methanol in the catalyst were obtained by the finite element method in MATLAB. The reaction–diffusion model was verified by the global kinetics data. The calculation data agreed well with the experimental data, so the model can be used to describe the processes of reaction and diffusion in the cylindrical-shaped catalyst. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Dehydration of methanol to dimethyl ether (DME) over a commercial γ-Al2O3 catalyst was studied at the temperature interval 513–613 K, liquid hourly space velocity (LHSV) of 0.9–6.0 h−1 and pressures between 0.1 and 1.0 MPa. The effect of different operation conditions on the dehydration of methanol was investigated in an isothermal fixed bed reactor. A kinetic equation which describes a Langmuir–Hinshelwood surface controlled reaction with dissociative adsorption of methanol was found to fit the experimental results quite well. An activation energy of 62.4 kJ/mol was obtained for the catalyst. A two-dimensional reaction–diffusion model was established for a cylindrical-shaped methanol dehydration catalyst. The internal effectiveness factor and the concentration distribution of methanol in the catalyst were obtained by the finite element method in MATLAB. The reaction–diffusion model was verified by the global kinetics data. The calculation data agreed well with the experimental data, so the model can be used to describe the processes of reaction and diffusion in the cylindrical-shaped catalyst. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21785" xmlns="http://purl.org/rss/1.0/"><title>Optimisation of the operational parameters during a biological nitrification process using response surface methodology</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21785</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Optimisation of the operational parameters during a biological nitrification process using response surface methodology</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">R. Darvishi Cheshmeh Soltani, A. Rezaee, A.R. Khataee, H. Godini</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-24T15:09:10.380582-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21785</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21785</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21785</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Biotechnology, Biochemical and Biomedical Engineering</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 main aim of this study was to determine the optimal operational parameters for a biological nitrification process. For this reason, a batch mode biological nitrification filled with acclimated sludge was used to remove ammonium from synthetic wastewater. Increasing the initial ammonium concentration from 50 to 300 mg NH<sub>4</sub>-N/L within 67 days led to a decrease in the removal efficiency of ammonium from 97.2% to 57.3%, which is equivalent to increasing the specific ammonium oxidation from 1.09 to 3.85 mg NH<sub>4</sub>-N/g MLVSS/h. Response surface methodology (RSM) based on central composite design (CCD) was used to evaluate the interactive effects of the three main parameters, including the sodium bicarbonate/ammonium chloride ratio, air flow rate and the reaction time, on the removal of ammonium. For the highest ammonium removal of 98.7%, the optimum sodium bicarbonate/ammonium chloride ratio, air flow rate and reaction time were identified to be 3.48, 3.44 vvm (volume air per volume reactor per minute) and 24.65 h, respectively, based on an initial ammonium concentration of 200 mg NH<sub>4</sub>-N/L. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

The main aim of this study was to determine the optimal operational parameters for a biological nitrification process. For this reason, a batch mode biological nitrification filled with acclimated sludge was used to remove ammonium from synthetic wastewater. Increasing the initial ammonium concentration from 50 to 300 mg NH4-N/L within 67 days led to a decrease in the removal efficiency of ammonium from 97.2% to 57.3%, which is equivalent to increasing the specific ammonium oxidation from 1.09 to 3.85 mg NH4-N/g MLVSS/h. Response surface methodology (RSM) based on central composite design (CCD) was used to evaluate the interactive effects of the three main parameters, including the sodium bicarbonate/ammonium chloride ratio, air flow rate and the reaction time, on the removal of ammonium. For the highest ammonium removal of 98.7%, the optimum sodium bicarbonate/ammonium chloride ratio, air flow rate and reaction time were identified to be 3.48, 3.44 vvm (volume air per volume reactor per minute) and 24.65 h, respectively, based on an initial ammonium concentration of 200 mg NH4-N/L. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21788" xmlns="http://purl.org/rss/1.0/"><title>Effect of liquid viscosity on hydrodynamics and bubble behaviour of an external-loop airlift reactor</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21788</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of liquid viscosity on hydrodynamics and bubble behaviour of an external-loop airlift reactor</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Qian Wu, Xuekui Wang, Tiefeng Wang, Mei Han, Zuoliang Sha, Jinfu Wang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-24T15:09:06.569714-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21788</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21788</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21788</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena, Fluid Dynamics and Thermodynamics</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 liquid viscosity on hydrodynamics and bubble behaviour of an external-loop airlift reactor within air–water system were studied by an electrical conductivity probe. Carboxyl methyl cellulose (CMC) was used to change liquid viscosity (1.00–51.25 cP). Gas holdup increased with superficial gas velocity increasing, as well as bubble Sauter diameter and bubble rise velocity. With liquid viscosity increasing, average gas holdup increased first then decreased, while bubble Sauter diameter was opposite, with critical viscosity <em>µ</em><sub>l</sub> ≈ 3.7 cP. The cross-sectional average bubble Sauter diameter increased obviously after <em>µ</em><sub>l</sub> &gt; 3.7 cP, and its size distribution was wider within the higher viscosity. Bubble rise velocity increased significantly and nearly unchanged after <em>µ</em><sub>l</sub> &gt; 10.3 cP. Gas holdup first increased then remained unchanged with the axial height increasing. The radial profile of local gas holdup presented a central peak distribution, and the value at inlet was smaller than that at the higher position. Average gas holdup was correlated greatly with superficial gas velocity and liquid viscosity. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

The effect of liquid viscosity on hydrodynamics and bubble behaviour of an external-loop airlift reactor within air–water system were studied by an electrical conductivity probe. Carboxyl methyl cellulose (CMC) was used to change liquid viscosity (1.00–51.25 cP). Gas holdup increased with superficial gas velocity increasing, as well as bubble Sauter diameter and bubble rise velocity. With liquid viscosity increasing, average gas holdup increased first then decreased, while bubble Sauter diameter was opposite, with critical viscosity µl ≈ 3.7 cP. The cross-sectional average bubble Sauter diameter increased obviously after µl &gt; 3.7 cP, and its size distribution was wider within the higher viscosity. Bubble rise velocity increased significantly and nearly unchanged after µl &gt; 10.3 cP. Gas holdup first increased then remained unchanged with the axial height increasing. The radial profile of local gas holdup presented a central peak distribution, and the value at inlet was smaller than that at the higher position. Average gas holdup was correlated greatly with superficial gas velocity and liquid viscosity. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21781" xmlns="http://purl.org/rss/1.0/"><title>Pressure drop optimisation in design of multi-stream plate-fin heat exchangers, considering variable physical properties</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21781</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Pressure drop optimisation in design of multi-stream plate-fin heat exchangers, considering variable physical properties</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Nassim Tahouni, Samira Miryahyaie, Fatemeh Joda, Hamid Reza Fallahi, Mohammad Hassan Panjeshahi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-24T15:09:03.918381-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21781</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21781</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21781</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Process Systems Engineering</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 modified method for the design of multi-stream plate-fin heat exchangers that considers variable physical properties is proposed in this paper. The new method, based on Pinch Technology, exploits the dependency of physical properties (heat capacity, viscosity, density and thermal conductivity) on temperature variations. A set of temperature correction factors based on variable physical properties is derived for the hot and cold streams of a multi-stream heat exchanger. This allows calculation of effective stream pressure drops, which can lead to a valid trade-off between operating and capital cost in the targeting stage. Accordingly, composite curves are constructed; based on the enthalpy intervals, the multi-stream heat exchanger is subdivided into a number of block sections. A plate-fin heat exchanger is then designed for each section by maximising the allowable effective pressure drops. Next, using a Genetic Algorithm, the method is completed in order to optimise the pressure drop of streams. Therefore, fin types for each individual stream are considered as optimising variables. By taking the variable physical properties of each stream into account and using the best fin selection, one can achieve accurate results in the design stage. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

A modified method for the design of multi-stream plate-fin heat exchangers that considers variable physical properties is proposed in this paper. The new method, based on Pinch Technology, exploits the dependency of physical properties (heat capacity, viscosity, density and thermal conductivity) on temperature variations. A set of temperature correction factors based on variable physical properties is derived for the hot and cold streams of a multi-stream heat exchanger. This allows calculation of effective stream pressure drops, which can lead to a valid trade-off between operating and capital cost in the targeting stage. Accordingly, composite curves are constructed; based on the enthalpy intervals, the multi-stream heat exchanger is subdivided into a number of block sections. A plate-fin heat exchanger is then designed for each section by maximising the allowable effective pressure drops. Next, using a Genetic Algorithm, the method is completed in order to optimise the pressure drop of streams. Therefore, fin types for each individual stream are considered as optimising variables. By taking the variable physical properties of each stream into account and using the best fin selection, one can achieve accurate results in the design stage. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21783" xmlns="http://purl.org/rss/1.0/"><title>Incorporating feedforward action into self-optimising control policies</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21783</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Incorporating feedforward action into self-optimising control policies</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Lia Maisarah Umar, Yi Cao, Vinay Kariwala</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-24T15:09:02.474125-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21783</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21783</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21783</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Process Systems Engineering</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 available methods for the selection of controlled variables (CVs), using the concept of self-optimising control (SOC), focus on finding CVs, which are held at constant setpoints using a feedback controller. In this paper, it is shown that better self-optimising properties can be achieved by incorporating feedforward action using measured disturbances in the SOC policies. The resulting operational policy allows the setpoints for CVs to be varied with measured disturbances, allowing for near-optimal operation in the presence of disturbances and uncertainties. The effectiveness of the proposed approach is demonstrated through its application to an exothermic reactor and a forced-circulation evaporator. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

The available methods for the selection of controlled variables (CVs), using the concept of self-optimising control (SOC), focus on finding CVs, which are held at constant setpoints using a feedback controller. In this paper, it is shown that better self-optimising properties can be achieved by incorporating feedforward action using measured disturbances in the SOC policies. The resulting operational policy allows the setpoints for CVs to be varied with measured disturbances, allowing for near-optimal operation in the presence of disturbances and uncertainties. The effectiveness of the proposed approach is demonstrated through its application to an exothermic reactor and a forced-circulation evaporator. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21758" xmlns="http://purl.org/rss/1.0/"><title>Cu-based mixed metal oxide catalysts for WGSR: Reduction kinetics and catalytic activity</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21758</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Cu-based mixed metal oxide catalysts for WGSR: Reduction kinetics and catalytic activity</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mohammad M. Hossain, Shakeel Ahmed</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-24T15:08:54.411617-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21758</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21758</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21758</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<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 communication reports the effects of Mn/Cr on the reducibility and catalytic activity of Cu–Fe–Mn and Cu–Fe–Cr mixed oxide catalysts for the water gas shift reaction (WGSR). The reduction kinetics of the mixed oxide catalysts is investigated using TPR data, nucleation/nuclei growth models, and a power law model. Based on the statistical indicators, it is concluded that a second-order power law model describes the reduction of all catalysts adequately. The estimated activation energy for the reduction of the Cu–Fe–Mn catalyst is low compared to the Cu–Fe–Cr catalyst. The TPR analysis of the catalysts reveals that the addition of Mn significantly improved the reducibility of Cu-oxide species, which is consistent with the low activation energy for reduction of the Cu–Fe–Mn catalyst. In a flow type reactor, the Cu–Fe–Mn catalyst showed highest CO conversion at around 220°C, achieving a high specific reaction rate compared to the Cu–Fe–Cr catalyst. The enhanced reducibility of Cu–Fe–Mn catalyst played the key role in the high conversion of CO. These results are comparable with the results obtained for a commercial Cu–ZnO/Al<sub>2</sub>O<sub>3</sub> catalyst, which was evaluated under the same reaction conditions. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

This communication reports the effects of Mn/Cr on the reducibility and catalytic activity of Cu–Fe–Mn and Cu–Fe–Cr mixed oxide catalysts for the water gas shift reaction (WGSR). The reduction kinetics of the mixed oxide catalysts is investigated using TPR data, nucleation/nuclei growth models, and a power law model. Based on the statistical indicators, it is concluded that a second-order power law model describes the reduction of all catalysts adequately. The estimated activation energy for the reduction of the Cu–Fe–Mn catalyst is low compared to the Cu–Fe–Cr catalyst. The TPR analysis of the catalysts reveals that the addition of Mn significantly improved the reducibility of Cu-oxide species, which is consistent with the low activation energy for reduction of the Cu–Fe–Mn catalyst. In a flow type reactor, the Cu–Fe–Mn catalyst showed highest CO conversion at around 220°C, achieving a high specific reaction rate compared to the Cu–Fe–Cr catalyst. The enhanced reducibility of Cu–Fe–Mn catalyst played the key role in the high conversion of CO. These results are comparable with the results obtained for a commercial Cu–ZnO/Al2O3 catalyst, which was evaluated under the same reaction conditions. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21786" xmlns="http://purl.org/rss/1.0/"><title>Preparation of microporous activated carbon from Aegle marmelos fruit shell by KOH activation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21786</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Preparation of microporous activated carbon from Aegle marmelos fruit shell by KOH activation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ramakrishna Gottipati, Susmita Mishra</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-24T15:08:50.705494-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21786</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21786</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21786</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Environment, Renewable Resources, Green Processes</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>Activated carbon (AC) is well-known for its unique properties; hence, the search for new precursors and the investigation of new methods for the preparation of AC is still drawing attention of many researchers. In the present work, microporous AC was prepared from <em>Aegle marmelos</em> fruit shell (AMFS) by potassium hydroxide (KOH) activation. The effect of process parameters such as impregnation ratio, carbonisation temperature and holding time on porous characteristics was investigated. The porous characteristics of prepared AC samples were analysed by N<sub>2</sub> adsorption–desorption isotherms, and it was found that the isotherms obtained resemble typical microporous solids (Type-I). The Langmuir surface area and total pore volume of the sample prepared at optimum conditions were found to be 937 m<sup>2</sup>/g and 0.33 cm<sup>3</sup>/g, respectively. The contribution of micropores to the porous characteristics of the prepared AC is very much appreciable, and about 97% of the total surface area and pore volume is attained by micropores. Pore size distribution (PSD) by Dubinin–Astakhov (DA) and micro-pore (MP) methods confirmed the presence of micropores to a great extent with insignificant mesoporosity. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Activated carbon (AC) is well-known for its unique properties; hence, the search for new precursors and the investigation of new methods for the preparation of AC is still drawing attention of many researchers. In the present work, microporous AC was prepared from Aegle marmelos fruit shell (AMFS) by potassium hydroxide (KOH) activation. The effect of process parameters such as impregnation ratio, carbonisation temperature and holding time on porous characteristics was investigated. The porous characteristics of prepared AC samples were analysed by N2 adsorption–desorption isotherms, and it was found that the isotherms obtained resemble typical microporous solids (Type-I). The Langmuir surface area and total pore volume of the sample prepared at optimum conditions were found to be 937 m2/g and 0.33 cm3/g, respectively. The contribution of micropores to the porous characteristics of the prepared AC is very much appreciable, and about 97% of the total surface area and pore volume is attained by micropores. Pore size distribution (PSD) by Dubinin–Astakhov (DA) and micro-pore (MP) methods confirmed the presence of micropores to a great extent with insignificant mesoporosity. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21789" xmlns="http://purl.org/rss/1.0/"><title>Comparative analysis of mathematical models for supercritical extraction simulation from industrially valuable Lamiaceae herbs</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21789</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Comparative analysis of mathematical models for supercritical extraction simulation from industrially valuable Lamiaceae herbs</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Marko Stamenic, Jasna Ivanovic, Slavica Grujic, Stoja Milovanovic, Irena Zizovic, Slobodan Petrovic</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-24T15:08:49.142956-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21789</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21789</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21789</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Process Systems Engineering</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 present study was aimed to compare different mathematical models used to simulate process of supercritical extraction from commercially important Lamiaceae herbs. Supercritical extractions with carbon dioxide from rosemary, sage, thyme and lavender originated from the southern Balkan region were performed at 10 MPa and 40°C. Obtained extraction curves were simulated by the model based on the heat transfer analogy, Sovova's model and the model on the micro-scale. The models were used to analyse mass transfer phenomena and to quantify mass transfer parameters in the fluid and/or solid phase as well as the solubility of the solute in supercritical phase. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

The present study was aimed to compare different mathematical models used to simulate process of supercritical extraction from commercially important Lamiaceae herbs. Supercritical extractions with carbon dioxide from rosemary, sage, thyme and lavender originated from the southern Balkan region were performed at 10 MPa and 40°C. Obtained extraction curves were simulated by the model based on the heat transfer analogy, Sovova's model and the model on the micro-scale. The models were used to analyse mass transfer phenomena and to quantify mass transfer parameters in the fluid and/or solid phase as well as the solubility of the solute in supercritical phase. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21787" xmlns="http://purl.org/rss/1.0/"><title>Simulation of methane catalytic cracking in a bubbling fluidised bed</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21787</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Simulation of methane catalytic cracking in a bubbling fluidised bed</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ashraf Amin, Eric Croiset, William Epling</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-24T15:08:47.523402-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21787</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21787</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21787</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, Chemical Kinetics and Catalysis</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 three-phase bubbling fluidised bed model has been developed to simulate and predict the performance of a methane catalytic cracking fluidised bed reactor, using Ni/(porous and non-porous) Al<sub>2</sub>O<sub>3</sub> catalysts, under relevant conditions. The model includes the chemistry and hydrodynamics occurring within the fluidised bed reactor. Methane cracking kinetics, developed in a previous work using a thermo balance, was used in the model. The model predictions were compared to the results from an experimental study carried out in a lab-scale fluidised bed. Good fit between experimental data and the model was obtained under a wide range of reaction conditions. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

A three-phase bubbling fluidised bed model has been developed to simulate and predict the performance of a methane catalytic cracking fluidised bed reactor, using Ni/(porous and non-porous) Al2O3 catalysts, under relevant conditions. The model includes the chemistry and hydrodynamics occurring within the fluidised bed reactor. Methane cracking kinetics, developed in a previous work using a thermo balance, was used in the model. The model predictions were compared to the results from an experimental study carried out in a lab-scale fluidised bed. Good fit between experimental data and the model was obtained under a wide range of reaction conditions. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21790" xmlns="http://purl.org/rss/1.0/"><title>Analysis of natural convection in a nanofluid-filled triangular enclosure induced by cold and hot sources on the walls using stabilised MLPG method</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21790</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Analysis of natural convection in a nanofluid-filled triangular enclosure induced by cold and hot sources on the walls using stabilised MLPG method</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ali Arefmanesh, Mehdi Nikfar</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-24T15:08:44.226888-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21790</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21790</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21790</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena, Fluid Dynamics and Thermodynamics</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 stabilised meshless local Petrov–Galerkin (MLPG) method with unity as the test function is extended to simulate the buoyancy-driven fluid flow and heat transfer in a right-angled, triangular enclosure filled with a nanofluid composed of a mixture of Al<sub>2</sub>O<sub>3</sub> spherical nanoparticles in water. A cold source with a constant temperature <em>T</em><sub>c</sub> and a hot source with a constant temperature <em>T</em><sub>h</sub> are placed along the left and bottom walls of the cavity, respectively, with a differential temperature difference between <em>T</em><sub>c</sub> and <em>T</em><sub>h</sub> so that <em>T</em><sub>h</sub> &gt; <em>T</em><sub>c</sub>. The simulations performed in this study are based on the stream function–vorticity formulation. The moving least-squares interpolations of the field variables are employed in these MLPG numerical calculations. A streamline upwind technique is employed to obtain stable solutions for high Rayleigh numbers. A parametric study is performed, and the effects of the Rayleigh number, the locations of the cold and hot sources on the respective cavity walls, and the volume fraction of the nanoparticles on the fluid flow and heat transfer inside the cavity are investigated. The results show that the average Nusselt number is generally an increasing function of the volume fraction of the nanoparticles. Moreover, it is concluded from the results that the locations of the cold and hot sources on the respective cavity walls have a significant effect on the flow and temperature fields inside the enclosure. In general, the maximum average Nusselt number occurs when the centres of the cold and hot sources are at <em>Y</em><sub>s</sub> = 0.167 and <em>X</em><sub>s</sub> = 0.167, respectively, while the average Nusselt number is minimum for <em>Y</em><sub>s</sub> = 0.833 and <em>X</em><sub>s</sub> = 0.833. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

A stabilised meshless local Petrov–Galerkin (MLPG) method with unity as the test function is extended to simulate the buoyancy-driven fluid flow and heat transfer in a right-angled, triangular enclosure filled with a nanofluid composed of a mixture of Al2O3 spherical nanoparticles in water. A cold source with a constant temperature Tc and a hot source with a constant temperature Th are placed along the left and bottom walls of the cavity, respectively, with a differential temperature difference between Tc and Th so that Th &gt; Tc. The simulations performed in this study are based on the stream function–vorticity formulation. The moving least-squares interpolations of the field variables are employed in these MLPG numerical calculations. A streamline upwind technique is employed to obtain stable solutions for high Rayleigh numbers. A parametric study is performed, and the effects of the Rayleigh number, the locations of the cold and hot sources on the respective cavity walls, and the volume fraction of the nanoparticles on the fluid flow and heat transfer inside the cavity are investigated. The results show that the average Nusselt number is generally an increasing function of the volume fraction of the nanoparticles. Moreover, it is concluded from the results that the locations of the cold and hot sources on the respective cavity walls have a significant effect on the flow and temperature fields inside the enclosure. In general, the maximum average Nusselt number occurs when the centres of the cold and hot sources are at Ys = 0.167 and Xs = 0.167, respectively, while the average Nusselt number is minimum for Ys = 0.833 and Xs = 0.833. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21784" xmlns="http://purl.org/rss/1.0/"><title>Adsorption isotherms, kinetics and mechanism of Pb(II) ions removal from aqueous solution using chemically modified agricultural waste</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21784</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Adsorption isotherms, kinetics and mechanism of Pb(II) ions removal from aqueous solution using chemically modified agricultural waste</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">P. Senthil Kumar, C. Senthamarai, A.S.L. Sai Deepthi, R. Bharani</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-24T15:08:43.080958-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21784</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21784</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21784</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separation Processes</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 removal of Pb(II) ions from aqueous solution by chemically surface modified <em>Strychnos potatorum</em> seeds (SMSP) was investigated. The surface modification of the adsorbent was confirmed by the FTIR and SEM analyses. The Freundlich adsorption isotherm model provides a better fit to the adsorption isotherm data. The maximum adsorption capacity of SMSP for Pb(II) ions was found to be 166.67 mg/g at optimum conditions of pH 5.0, contact time of 30 min, SMSP dosage of 2 g/L and temperature of 30°C. The adsorption kinetics for Pb(II) ions removal by the SMSP follows the pseudo-second order kinetic model. Adsorption mechanism of Pb(II) ions onto the SMSP was explained with the intraparticle diffusion, Boyd kinetic and Shrinking core models (SCM). The effective diffusivity values were calculated from the Boyd kinetic model: 7.723 × 10<sup>−12</sup>, 8.464 × 10<sup>−12</sup>, 6.877 × 10<sup>−12</sup>, 8.358 × 10<sup>−12</sup> and 6.983 × 10<sup>−12</sup> m<sup>2</sup>/s for the initial Pb(II) ions concentration from 100 to 500 mg/L, respectively. The diffusivity values were estimated from the SCM: 8.901 × 10<sup>−9</sup>, 8.586 × 10<sup>−9</sup>, 8.359 × 10<sup>−9</sup>, 5.368 × 10<sup>−9</sup> and 4.318 × 10<sup>−9</sup> m<sup>2</sup>/s for the initial Pb(II) ions concentration from 100 to 500 mg/L, respectively. The results suggest that SMSP can be used as an effective low-cost adsorbent for the Pb(II) ions removal. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

The removal of Pb(II) ions from aqueous solution by chemically surface modified Strychnos potatorum seeds (SMSP) was investigated. The surface modification of the adsorbent was confirmed by the FTIR and SEM analyses. The Freundlich adsorption isotherm model provides a better fit to the adsorption isotherm data. The maximum adsorption capacity of SMSP for Pb(II) ions was found to be 166.67 mg/g at optimum conditions of pH 5.0, contact time of 30 min, SMSP dosage of 2 g/L and temperature of 30°C. The adsorption kinetics for Pb(II) ions removal by the SMSP follows the pseudo-second order kinetic model. Adsorption mechanism of Pb(II) ions onto the SMSP was explained with the intraparticle diffusion, Boyd kinetic and Shrinking core models (SCM). The effective diffusivity values were calculated from the Boyd kinetic model: 7.723 × 10−12, 8.464 × 10−12, 6.877 × 10−12, 8.358 × 10−12 and 6.983 × 10−12 m2/s for the initial Pb(II) ions concentration from 100 to 500 mg/L, respectively. The diffusivity values were estimated from the SCM: 8.901 × 10−9, 8.586 × 10−9, 8.359 × 10−9, 5.368 × 10−9 and 4.318 × 10−9 m2/s for the initial Pb(II) ions concentration from 100 to 500 mg/L, respectively. The results suggest that SMSP can be used as an effective low-cost adsorbent for the Pb(II) ions removal. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21779" xmlns="http://purl.org/rss/1.0/"><title>Cold model testing of a re-circulating fluidised bed reactor working in alternate aeration—fuel burning cycles for chemical looping</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21779</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Cold model testing of a re-circulating fluidised bed reactor working in alternate aeration—fuel burning cycles for chemical looping</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Raman Sharma, Arnaud Delabarre, Babu Alappat</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-24T15:08:41.459095-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21779</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21779</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21779</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separation Processes</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 re-circulating fluidised bed (RCFB) reactor is proposed here for gaseous fuel combustion using chemical-looping combustion (CLC). A single RCFB reactor was operated in alternate oxidation and reduction cycles for simulating the interconnected reactors arrangement for CLC. For this, a Perspex made transparent, concentric, semicircular cold model of RCFB reactor was used with three grades of Indian Standard sand. Operational parameters like bed inventory, pressure drop, particle size, suspension density, solid circulation rate, bed voidage and fluidisation gas velocity were studied to how they affect the performance of the RCFB reactor. The solid circulation rate has been found to increase with the increase in the bed inventory. Proper solid circulation rate is very much required for proper heat and mass transfer in an interconnected fluidised bed reactors system. The bed voidage is observed to be high during the aeration cycle and low during the reduction cycle. A high bed voidage during the oxidation cycle is appropriate for the fast oxidation reaction of the metal oxides. However, a low bed voidage is required for proper heat transfer for an endothermic reduction reaction in the fuel reactor. Suspension density in the downcomer of the RCFB reactor has been found to be increasing with bed inventory for both the oxidation and reduction cycles, which is good for the bed-to-wall heat transfer. A good observed solid circulation rate, operating voidage and suspension density add to the capability of RCFB to run CLC. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

A re-circulating fluidised bed (RCFB) reactor is proposed here for gaseous fuel combustion using chemical-looping combustion (CLC). A single RCFB reactor was operated in alternate oxidation and reduction cycles for simulating the interconnected reactors arrangement for CLC. For this, a Perspex made transparent, concentric, semicircular cold model of RCFB reactor was used with three grades of Indian Standard sand. Operational parameters like bed inventory, pressure drop, particle size, suspension density, solid circulation rate, bed voidage and fluidisation gas velocity were studied to how they affect the performance of the RCFB reactor. The solid circulation rate has been found to increase with the increase in the bed inventory. Proper solid circulation rate is very much required for proper heat and mass transfer in an interconnected fluidised bed reactors system. The bed voidage is observed to be high during the aeration cycle and low during the reduction cycle. A high bed voidage during the oxidation cycle is appropriate for the fast oxidation reaction of the metal oxides. However, a low bed voidage is required for proper heat transfer for an endothermic reduction reaction in the fuel reactor. Suspension density in the downcomer of the RCFB reactor has been found to be increasing with bed inventory for both the oxidation and reduction cycles, which is good for the bed-to-wall heat transfer. A good observed solid circulation rate, operating voidage and suspension density add to the capability of RCFB to run CLC. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21776" xmlns="http://purl.org/rss/1.0/"><title>Heavy water enrichment by thermal diffusion in the flat-plate frazier scheme with column heights increased at a constant ratio for improved performance</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21776</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Heavy water enrichment by thermal diffusion in the flat-plate frazier scheme with column heights increased at a constant ratio for improved performance</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ching-Chun Hsu, Ho-Ming Yeh</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-24T15:08:40.986325-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21776</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21776</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21776</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separation Processes</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 study investigates heavy water enrichment using the Frazier scheme of flat-plate thermal diffusion columns with the column number adjusted and the column heights varied at a constant ratio with the total sum of column heights fixed. The equations for predicting the best number of columns and the best column-height ratio for maximum separation are derived. Considerable improvement in performance is obtainable if the column-height ratio and/or column number in a modified Frazier scheme are properly assigned, instead of using the conventional Frazier scheme of uniform column height with the same total sum of column heights. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

This study investigates heavy water enrichment using the Frazier scheme of flat-plate thermal diffusion columns with the column number adjusted and the column heights varied at a constant ratio with the total sum of column heights fixed. The equations for predicting the best number of columns and the best column-height ratio for maximum separation are derived. Considerable improvement in performance is obtainable if the column-height ratio and/or column number in a modified Frazier scheme are properly assigned, instead of using the conventional Frazier scheme of uniform column height with the same total sum of column heights. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21778" xmlns="http://purl.org/rss/1.0/"><title>Just-suspended agitation of solid mixtures</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21778</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Just-suspended agitation of solid mixtures</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Tianxin Bao, Kevin J. Myers, Eric E. Janz, Julian B. Fasano</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-24T15:08:14.380144-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21778</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21778</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21778</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Industrial Applications of Chemical Engineering Principles</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>For binary solid mixtures, the mixture just-suspended speed is predicted with reasonable accuracy from the sum of powers to suspend the solids individually. Exceptions to this behaviour occur for mixtures of low-density solids and for mixtures involving a small, high-density solid. For these systems, summing the powers required to individually suspend the solids over-predicts the mixture just-suspended speed. Limited testing of ternary solid mixtures indicates that summing the powers required to individually suspend the solids also predicts the just-suspended speed in these more complex systems. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

For binary solid mixtures, the mixture just-suspended speed is predicted with reasonable accuracy from the sum of powers to suspend the solids individually. Exceptions to this behaviour occur for mixtures of low-density solids and for mixtures involving a small, high-density solid. For these systems, summing the powers required to individually suspend the solids over-predicts the mixture just-suspended speed. Limited testing of ternary solid mixtures indicates that summing the powers required to individually suspend the solids also predicts the just-suspended speed in these more complex systems. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21769" xmlns="http://purl.org/rss/1.0/"><title>Activated carbon prepared from canadian oil sands coke by CO2 activation: II. adsorption of metallic ions and organic constituents from oil sands tailings water</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21769</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Activated carbon prepared from canadian oil sands coke by CO2 activation: II. adsorption of metallic ions and organic constituents from oil sands tailings water</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Arash Karimi, Olivier Thinon, Joseph Fournier, Josephine M. Hill</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-24T08:42:43.427859-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21769</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21769</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21769</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<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>Oil sands coke was activated with CO<sub>2</sub> at 900°C in a tubular fixed bed reactor. Samples activated in a CO<sub>2</sub> stream with 50% air contained a significant number of functional groups. Some activated samples were post-oxidised in air at 350°C to increase their surface functionality. Post-oxidation was necessary for the adsorption of ferric cations by the coke samples activated, except for the sample activated with 50% air. However, non-oxidised samples were also able to adsorb molybdate anions. Both organic and inorganic constituents of oil sands tailings water were successfully removed, but some inorganic species leached into water. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Oil sands coke was activated with CO2 at 900°C in a tubular fixed bed reactor. Samples activated in a CO2 stream with 50% air contained a significant number of functional groups. Some activated samples were post-oxidised in air at 350°C to increase their surface functionality. Post-oxidation was necessary for the adsorption of ferric cations by the coke samples activated, except for the sample activated with 50% air. However, non-oxidised samples were also able to adsorb molybdate anions. Both organic and inorganic constituents of oil sands tailings water were successfully removed, but some inorganic species leached into water. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21772" xmlns="http://purl.org/rss/1.0/"><title>Non-ideal metal binding model for Cr(III) sorption using Spirulina platensis biomass: Experimental and theoretical approach</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21772</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Non-ideal metal binding model for Cr(III) sorption using Spirulina platensis biomass: Experimental and theoretical approach</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mahesh Kumar Gagrai, Chandan Das, Animes Kumar Golder</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-24T08:42:28.043505-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21772</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21772</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21772</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Environment, Renewable Resources, Green Processes</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>Removal of Cr(III) from aqueous solution using <em>Spirulina</em> biomass was studied in a batch experiment. <em>Spirulina</em> biomass was characterised before and after Cr(III) sorption using FTIR, SEM and potentiometric titration. The effects of experimental parameters such as solution pH, contact time, biomass dose, initial Cr(III) concentration and temperature were studied. pH had significant influence on Cr(III) uptake capacity of biomass. The optimum equilibrium solution pH was found as 6.2. Biosorption efficiency decreased at higher temperature. A simple proton binding model was investigated for the quantitative determination of acid–base characteristics of <em>Spirulina</em>. The dissociation constants (p<em>K</em><sub>a</sub>) of 1.19, 2.87 and 8.07 mol L<sup>−1</sup> were estimated, which correspond to carboxylic, phosphatic and amine groups, respectively. A modified metal binding model was then tested, and Cr(III) binding constants (<em>K</em><sub><em>θ</em></sub>) of 80.9, 3.9 × 10<sup>3</sup> and 3.5 × 10<sup>4</sup> L mol<sup>−1</sup> were found for carboxylic, phosphatic and amine groups, respectively. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Removal of Cr(III) from aqueous solution using Spirulina biomass was studied in a batch experiment. Spirulina biomass was characterised before and after Cr(III) sorption using FTIR, SEM and potentiometric titration. The effects of experimental parameters such as solution pH, contact time, biomass dose, initial Cr(III) concentration and temperature were studied. pH had significant influence on Cr(III) uptake capacity of biomass. The optimum equilibrium solution pH was found as 6.2. Biosorption efficiency decreased at higher temperature. A simple proton binding model was investigated for the quantitative determination of acid–base characteristics of Spirulina. The dissociation constants (pKa) of 1.19, 2.87 and 8.07 mol L−1 were estimated, which correspond to carboxylic, phosphatic and amine groups, respectively. A modified metal binding model was then tested, and Cr(III) binding constants (Kθ) of 80.9, 3.9 × 103 and 3.5 × 104 L mol−1 were found for carboxylic, phosphatic and amine groups, respectively. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21774" xmlns="http://purl.org/rss/1.0/"><title>Activated carbon prepared from Canadian oil sands coke by CO2 activation: I. trends in pore development and the effect of pre-oxidation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21774</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Activated carbon prepared from Canadian oil sands coke by CO2 activation: I. trends in pore development and the effect of pre-oxidation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Arash Karimi, Olivier Thinon, Joseph Fournier, Josephine M. Hill</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-31T10:50:56.369554-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21774</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21774</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21774</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Environment, Renewable Resources, Green Processes</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>Oil sands coke is a byproduct of oil sands upgrading, which potentially can be used for the production of low cost activated carbons. Activation of oil sands delayed coke was performed by partial CO<sub>2</sub>-gasification in a tubular fixed bed reactor at 900°C. Pore development during activation initially proceeded almost exclusively by micro-pore formation, and the reaction appeared to follow a shrinking core model. Surface areas up to 646 m<sup>2</sup>/g were obtained, and coarser particles reached lower maximum surface areas at lower levels of burn-off than finer particles. Pre-oxidation in air at 270°C resulted in higher maximum surface areas. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Oil sands coke is a byproduct of oil sands upgrading, which potentially can be used for the production of low cost activated carbons. Activation of oil sands delayed coke was performed by partial CO2-gasification in a tubular fixed bed reactor at 900°C. Pore development during activation initially proceeded almost exclusively by micro-pore formation, and the reaction appeared to follow a shrinking core model. Surface areas up to 646 m2/g were obtained, and coarser particles reached lower maximum surface areas at lower levels of burn-off than finer particles. Pre-oxidation in air at 270°C resulted in higher maximum surface areas. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21775" xmlns="http://purl.org/rss/1.0/"><title>Colloidal interaction and connectionist modelling of protein osmotic pressure and the effect of physicochemical properties</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21775</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Colloidal interaction and connectionist modelling of protein osmotic pressure and the effect of physicochemical properties</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Amin Reza Rajabzadeh, Sohrab Zendehboudi, Ali Lohi, Ali Elkamel</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-31T10:50:53.445055-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21775</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21775</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21775</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Biotechnology, Biochemical and Biomedical Engineering</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 proper knowledge of the osmotic pressure and thermodynamic behaviour of protein solutions is vital for designing an efficient protein separation process. It is also of great importance to develop a rapid and inexpensive technique to accurately estimate the protein osmotic pressure. A connectionist model to estimate the osmotic pressure of bovine serum albumin (BSA) in terms of pH, ionic strength and BSA concentration is proposed in this paper. Osmotic pressure of BSA is also modelled through the application of a colloidal interaction approach. Molecular interaction forces such as electrostatic, London–van der Waals and hydration along with entropy pressure are considered in the colloidal model to predict the BSA osmotic pressure. The advantages and disadvantages of both modelling approaches are discussed, and a hybrid modelling scheme is proposed for further investigations. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

A proper knowledge of the osmotic pressure and thermodynamic behaviour of protein solutions is vital for designing an efficient protein separation process. It is also of great importance to develop a rapid and inexpensive technique to accurately estimate the protein osmotic pressure. A connectionist model to estimate the osmotic pressure of bovine serum albumin (BSA) in terms of pH, ionic strength and BSA concentration is proposed in this paper. Osmotic pressure of BSA is also modelled through the application of a colloidal interaction approach. Molecular interaction forces such as electrostatic, London–van der Waals and hydration along with entropy pressure are considered in the colloidal model to predict the BSA osmotic pressure. The advantages and disadvantages of both modelling approaches are discussed, and a hybrid modelling scheme is proposed for further investigations. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21766" xmlns="http://purl.org/rss/1.0/"><title>Composite planning and scheduling algorithm addressing intra-period infeasibilities of gasoline blend planning models</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21766</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Composite planning and scheduling algorithm addressing intra-period infeasibilities of gasoline blend planning models</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">V. Mahalec, A. Thakral</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-31T10:50:50.393432-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21766</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21766</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21766</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<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>Multi-period planning models result in solutions which are feasible at the boundaries of the periods but may be infeasible within the periods. The composite algorithm presented here (i) solves coarse multi-period MILP model structure for production planning; (ii) sequences operations via a genetic algorithm to minimise switching; (iii) verifies schedule feasibility via agent-based simulation and local logical decision making; and (iv) if infeasible, re-partitions the time horizon into multi-periods and resolves from (i) until feasible. Application of the algorithm to gasoline blending illustrates its effectiveness in computing feasible plans and schedules for such systems. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Multi-period planning models result in solutions which are feasible at the boundaries of the periods but may be infeasible within the periods. The composite algorithm presented here (i) solves coarse multi-period MILP model structure for production planning; (ii) sequences operations via a genetic algorithm to minimise switching; (iii) verifies schedule feasibility via agent-based simulation and local logical decision making; and (iv) if infeasible, re-partitions the time horizon into multi-periods and resolves from (i) until feasible. Application of the algorithm to gasoline blending illustrates its effectiveness in computing feasible plans and schedules for such systems. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21770" xmlns="http://purl.org/rss/1.0/"><title>Equal consistency spraying and flow field characteristics of spraying water pipe</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21770</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Equal consistency spraying and flow field characteristics of spraying water pipe</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jin-Song Zeng, Ke-Fu Chen, Yu-Cheng Feng, Wang Wei, De-Tao Liu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-31T10:50:48.738082-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21770</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21770</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21770</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<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>As one of the key parts of discharging system in the diluted zone at the bottom of high consistency bleaching tower, the spraying water pipe would be used to dilute the pulp uniformly while it was rotating, with a range from 0 to 90 rpm. Fluid dynamics of the three kinds of spraying water pipes such as straight-shaped, spindle-shaped and waist-shaped were studied by performing computational fluid dynamics (CFD) simulations and particle image velocimetry (PIV) measurements. Simulated velocity fields were compared with experiment PIV data. The results from the simulations and experiments are in good agreement. The works show that CFD simulations using the Realisable <em>κ</em>–<em>ε</em> model combined with the MRF technique can predict the hydrodynamic characteristics in industrial scales spraying water pipes. Spindle-shaped spraying water pipe would be better finished equal consistency spraying water. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

As one of the key parts of discharging system in the diluted zone at the bottom of high consistency bleaching tower, the spraying water pipe would be used to dilute the pulp uniformly while it was rotating, with a range from 0 to 90 rpm. Fluid dynamics of the three kinds of spraying water pipes such as straight-shaped, spindle-shaped and waist-shaped were studied by performing computational fluid dynamics (CFD) simulations and particle image velocimetry (PIV) measurements. Simulated velocity fields were compared with experiment PIV data. The results from the simulations and experiments are in good agreement. The works show that CFD simulations using the Realisable κ–ε model combined with the MRF technique can predict the hydrodynamic characteristics in industrial scales spraying water pipes. Spindle-shaped spraying water pipe would be better finished equal consistency spraying water. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21767" xmlns="http://purl.org/rss/1.0/"><title>Effects of sweating temperature on the purification of phosphoric acid hemihydrate crystal in dry-sweating process</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21767</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effects of sweating temperature on the purification of phosphoric acid hemihydrate crystal in dry-sweating process</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Baoming Wang, Jun Li, Jianhong Luo, Kun Zhou, Yang Jin, Yabing Qi, Chunlei Ma</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-31T10:50:46.04855-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21767</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21767</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21767</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separation Processes</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 order to purify phosphoric acid hemihydrate (H<sub>3</sub>PO<sub>4</sub>·0.5H<sub>2</sub>O) crystal further, the effects of sweating time and sweating temperature on purification are investigated in a dry-sweating process. Experimental results indicate the content of Mg, As, Sb and Pb in the H<sub>3</sub>PO<sub>4</sub>·0.5H<sub>2</sub>O crystal decreases with increasing sweating time and sweating temperature during sweating process and show the same tendency to decrease with time at different sweating temperatures. The purification rate coefficients of H<sub>3</sub>PO<sub>4</sub>·0.5H<sub>2</sub>O crystals for Mg, As, Sb and Pb are determined. They increase with an increase in sweating temperature. The Arrhenius equation can be successfully used to describe the relationship between the purification rate coefficient and the absolute sweating temperature. The activation energy of sweating for Mg, As, Sb and Pb in the H<sub>3</sub>PO<sub>4</sub>·0.5H<sub>2</sub>O crystal are calculated using these experimental data. These values for Mg, As, Sb and Pb are 130.13, 193.59, 98.51 and 102.29 kJ mol<sup>−1</sup>, respectively. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

In order to purify phosphoric acid hemihydrate (H3PO4·0.5H2O) crystal further, the effects of sweating time and sweating temperature on purification are investigated in a dry-sweating process. Experimental results indicate the content of Mg, As, Sb and Pb in the H3PO4·0.5H2O crystal decreases with increasing sweating time and sweating temperature during sweating process and show the same tendency to decrease with time at different sweating temperatures. The purification rate coefficients of H3PO4·0.5H2O crystals for Mg, As, Sb and Pb are determined. They increase with an increase in sweating temperature. The Arrhenius equation can be successfully used to describe the relationship between the purification rate coefficient and the absolute sweating temperature. The activation energy of sweating for Mg, As, Sb and Pb in the H3PO4·0.5H2O crystal are calculated using these experimental data. These values for Mg, As, Sb and Pb are 130.13, 193.59, 98.51 and 102.29 kJ mol−1, respectively. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21768" xmlns="http://purl.org/rss/1.0/"><title>Nanoparticle-stabilised invert emulsion drilling fluids for deep-hole drilling of oil and gas</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21768</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Nanoparticle-stabilised invert emulsion drilling fluids for deep-hole drilling of oil and gas</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sushant Agarwal, Tran X. Phuoc, Yee Soong, Donald Martello, Rakesh K. Gupta</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-31T10:50:42.836212-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21768</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21768</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21768</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Nanotechnology</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>Invert emulsions are used to drill for oil and gas when good wellbore stability and high temperature tolerance are required. These drilling fluids contain a solid phase and two immiscible liquid phases stabilised with a polymeric surfactant. In ultra deep drilling, due to high temperature, the surfactant degrades causing phase separation. However, fine particles can be used as stabilisers, and the result is a Pickering emulsion. Here, we demonstrate that the use of a combination of hydrophobic nanoparticles and organically modified nanoclay results in stable water-in-oil invert emulsions model drilling fluids. These gel-like model fluids have the desired plastic viscosity and yield stress suitable for drilling fluid applications that can be modified by adjusting the nanoparticle-content. Aging experiments at 225°C showed that they also have high-temperature stability for demanding drilling operations. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Invert emulsions are used to drill for oil and gas when good wellbore stability and high temperature tolerance are required. These drilling fluids contain a solid phase and two immiscible liquid phases stabilised with a polymeric surfactant. In ultra deep drilling, due to high temperature, the surfactant degrades causing phase separation. However, fine particles can be used as stabilisers, and the result is a Pickering emulsion. Here, we demonstrate that the use of a combination of hydrophobic nanoparticles and organically modified nanoclay results in stable water-in-oil invert emulsions model drilling fluids. These gel-like model fluids have the desired plastic viscosity and yield stress suitable for drilling fluid applications that can be modified by adjusting the nanoparticle-content. Aging experiments at 225°C showed that they also have high-temperature stability for demanding drilling operations. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21762" xmlns="http://purl.org/rss/1.0/"><title>A novel analytical method predicts plug boundaries of Bingham plastic fluids for laminar flow through annulus</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21762</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A novel analytical method predicts plug boundaries of Bingham plastic fluids for laminar flow through annulus</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Alireza Bahadori, Gholamreza Zahedi, Sohrab Zendehboudi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-11-30T08:02:52.88192-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21762</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21762</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21762</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<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 Bingham plastic fluids, a central pre-yield or plug region exists in the middle of the concentric annular flow. In this region, the local shear stress is less than the dynamic yield stress, so the plug behaves like a rigid solid. This is the main feature that distinguishes the flow of a Bingham plastic fluid from that of a power law fluid. In this work, a simple-to-use correlation is developed to predict the boundaries of the plug of Bingham plastic fluids for laminar flow through annulus as a function of dimensionless yield stress and aspect ratio parameters for given values of the rheological constants, pressure gradient and the dimensions of the annulus. The results are found to be in excellent agreement with reported data in the literature with an average absolute deviation of less than 1.7%.</p></div>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The predictive tool is simple and straightforward and can be readily implemented in a standard spreadsheet program. The prime application of the method is as a quick-and-easy evaluation tool in engineering studies where plug boundaries of Bingham plastic fluids for laminar flow through annulus are being considered. The method may also serve as a benchmark in numerical and rigorous simulation studies. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

In Bingham plastic fluids, a central pre-yield or plug region exists in the middle of the concentric annular flow. In this region, the local shear stress is less than the dynamic yield stress, so the plug behaves like a rigid solid. This is the main feature that distinguishes the flow of a Bingham plastic fluid from that of a power law fluid. In this work, a simple-to-use correlation is developed to predict the boundaries of the plug of Bingham plastic fluids for laminar flow through annulus as a function of dimensionless yield stress and aspect ratio parameters for given values of the rheological constants, pressure gradient and the dimensions of the annulus. The results are found to be in excellent agreement with reported data in the literature with an average absolute deviation of less than 1.7%.
The predictive tool is simple and straightforward and can be readily implemented in a standard spreadsheet program. The prime application of the method is as a quick-and-easy evaluation tool in engineering studies where plug boundaries of Bingham plastic fluids for laminar flow through annulus are being considered. The method may also serve as a benchmark in numerical and rigorous simulation studies. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21763" xmlns="http://purl.org/rss/1.0/"><title>Effect of solids loading on agitator just-suspended speed</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21763</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of solids loading on agitator just-suspended speed</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Kevin J. Myers, Eric E. Janz, Julian B. Fasano</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-11-30T08:02:50.124114-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21763</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21763</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21763</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</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>Data taken with six solids at numerous Zwietering loadings ranging from near zero to 67 have been used to determine the just-suspended speed Zwietering loading exponent (<em>N</em><sub>js</sub> ∝ <em>X</em><sup><em>n</em></sup> where <em>n</em> is the Zwietering solids loading exponent). When only the loadings range similar to that studied by Zwietering [Zwietering, <em>Chem. Eng. Sci.</em> <b>1958</b>, <em>8</em>, 244] is considered (0 &lt; <em>X</em> &lt; 18), the solids loading exponent averaged over all solids is equal to 0.12, essentially the same as the 0.13 reported by Zwietering. However, when the entire loading range is considered (0 &lt; <em>X</em> ≤ 67), a higher average exponent of 0.17 is found and a single power-law correlation does not accurately describe the experimental data. A piecewise fit of the data indicates that the solids loading exponent increases from an average value of 0.097 at low solids loadings (0 &lt; <em>X</em> ≤ 5) to 0.22 at intermediate loadings (5 ≤ <em>X</em> ≤ 25) and 0.34 for the highest loadings (25 ≤ <em>X</em> ≤ 67). © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Data taken with six solids at numerous Zwietering loadings ranging from near zero to 67 have been used to determine the just-suspended speed Zwietering loading exponent (Njs ∝ Xn where n is the Zwietering solids loading exponent). When only the loadings range similar to that studied by Zwietering [Zwietering, Chem. Eng. Sci. 1958, 8, 244] is considered (0 &lt; X &lt; 18), the solids loading exponent averaged over all solids is equal to 0.12, essentially the same as the 0.13 reported by Zwietering. However, when the entire loading range is considered (0 &lt; X ≤ 67), a higher average exponent of 0.17 is found and a single power-law correlation does not accurately describe the experimental data. A piecewise fit of the data indicates that the solids loading exponent increases from an average value of 0.097 at low solids loadings (0 &lt; X ≤ 5) to 0.22 at intermediate loadings (5 ≤ X ≤ 25) and 0.34 for the highest loadings (25 ≤ X ≤ 67). © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21741" xmlns="http://purl.org/rss/1.0/"><title>Kinetic analysis and modelling of thermal degradation of perspex (PMMA) and perspex blend plastic waste</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21741</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Kinetic analysis and modelling of thermal degradation of perspex (PMMA) and perspex blend plastic waste</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Meshari AL-Harbi, Ahmad Alshaiban, Mohamed F. Yassin, Abdirashid Elmi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-11-13T09:24:26.873134-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21741</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21741</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21741</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Chemical Reaction Engineering</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 thermal decomposition of pure perspex and a mixture of 50% perspex and 50% poly(ethylene terephthalate; PET) was carried out between 295 and 325°C using a thermogravimetric analyser (TGA) in air and nitrogen (N<sub>2</sub>) atmosphere. The weight losses of decomposition products were measured during these experiments. The thermal degradation process is slower in inert atmosphere than air, where oxidation reaction expedites the decomposition process. Kinetic rate constants (<em>k</em>), pre-exponential factor (<em>A</em>) and activation energy (<em>E</em>) for both pure prespex and a blend of perspex/PET were calculated for both air and N<sub>2</sub> conditions. The thermal degradation process followed a third-order reaction in air and second-order in N<sub>2</sub>. A second-order (<em>n</em> = 2) model for the pyrolytic process based on simultaneous reactions was developed using experimental data for pure and blend. The pyrolytic products are gases, liquids, waxes, aromatics and char, which can be ultimately used as raw material and fuel in various applications. It is important to note that the addition of PET to perspex was found to suppress/inhibit the decomposition of perspex compared with pure perspex. Pre-exponential factor (<em>A</em>) and activation energy (<em>E</em>) values support such an observation. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

The thermal decomposition of pure perspex and a mixture of 50% perspex and 50% poly(ethylene terephthalate; PET) was carried out between 295 and 325°C using a thermogravimetric analyser (TGA) in air and nitrogen (N2) atmosphere. The weight losses of decomposition products were measured during these experiments. The thermal degradation process is slower in inert atmosphere than air, where oxidation reaction expedites the decomposition process. Kinetic rate constants (k), pre-exponential factor (A) and activation energy (E) for both pure prespex and a blend of perspex/PET were calculated for both air and N2 conditions. The thermal degradation process followed a third-order reaction in air and second-order in N2. A second-order (n = 2) model for the pyrolytic process based on simultaneous reactions was developed using experimental data for pure and blend. The pyrolytic products are gases, liquids, waxes, aromatics and char, which can be ultimately used as raw material and fuel in various applications. It is important to note that the addition of PET to perspex was found to suppress/inhibit the decomposition of perspex compared with pure perspex. Pre-exponential factor (A) and activation energy (E) values support such an observation. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21747" xmlns="http://purl.org/rss/1.0/"><title>Numerical modelling of convective vapour condensation with non-condensable gases between two coaxial vertical cylinders</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21747</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Numerical modelling of convective vapour condensation with non-condensable gases between two coaxial vertical cylinders</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Lazhar Merouani, Belkacem Zeghmati, Azeddine Belhamri</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-10-11T09:34:27.904021-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21747</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21747</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21747</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<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 problem of laminar film condensation from steam–gas mixtures between two coaxial cylinders is numerically analysed. A set of complete boundary layer equations is used to model simultaneous momentum, heat and mass transfer in the liquid film and the vapour–gas mixture. In order to locate accurately the liquid–mixture interface, a relevant change of coordinates is performed. Equations are solved using an implicit finite difference scheme. The liquid film thickness is determined from an iterative procedure based on the secant method. An analytical solution of the momentum equations of both phases at the end of condensation is also developed. Results presented include evolutions of field profiles and flow parameters from the inlet until the end of condensation. We also analyse the effects of the wall properties, the inlet conditions, the type of non-condensable gas, the size of the annular space and the convective cooling coefficient. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

A problem of laminar film condensation from steam–gas mixtures between two coaxial cylinders is numerically analysed. A set of complete boundary layer equations is used to model simultaneous momentum, heat and mass transfer in the liquid film and the vapour–gas mixture. In order to locate accurately the liquid–mixture interface, a relevant change of coordinates is performed. Equations are solved using an implicit finite difference scheme. The liquid film thickness is determined from an iterative procedure based on the secant method. An analytical solution of the momentum equations of both phases at the end of condensation is also developed. Results presented include evolutions of field profiles and flow parameters from the inlet until the end of condensation. We also analyse the effects of the wall properties, the inlet conditions, the type of non-condensable gas, the size of the annular space and the convective cooling coefficient. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21746" xmlns="http://purl.org/rss/1.0/"><title>Influence of pretreatment conditions on composition of liquid hydrolysate and subsequent enzymatic saccharification of remaining solids</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21746</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Influence of pretreatment conditions on composition of liquid hydrolysate and subsequent enzymatic saccharification of remaining solids</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ravi Dhabhai, Satyendra P. Chaurasia, Ajay K. Dalai</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-10-11T09:34:22.900536-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21746</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21746</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21746</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<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, the effect of dilute acid pretreatment was studied on the composition of liquid hydrolysate obtained after pretreatment by employing different combinations of process variables (temperature, time and acid concentration). The effect of pretreatment was also studied on subsequent enzymatic saccharification of remaining solids to obtain maximum yield of sugars. The efficiency of pretreatment was measured in terms of high-xylose and low-glucose yields, which was found most suitable at pretreatment conditions of 120°C, 120 min and 2% (v/v) acid concentration. With increased severity of pretreatment, xylose yield decreased with concomitant increase in glucose yield. The decrease in xylose yield was attributed to conversion into degradation products such as 5-hydroxylmethyl furfural (HMF) and acetic acid. The percentage of enzymatic saccharification increased with increased pretreatment severity. Saccharification of biomass pretreated at 180°C, 7 min and 0.5% (v/v) acid concentration produced the maximum glucose yield of saccharification of 352 g/kg dry matter, compared to just 97 g glucose/kg dry matter in the case of untreated biomass. The same pretreatment conditions resulted in maximum total sugar yield of pretreatment and saccharification of 459 g/kg dry matter, which was more than 67% of the total potential sugars in biomass. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

In the present work, the effect of dilute acid pretreatment was studied on the composition of liquid hydrolysate obtained after pretreatment by employing different combinations of process variables (temperature, time and acid concentration). The effect of pretreatment was also studied on subsequent enzymatic saccharification of remaining solids to obtain maximum yield of sugars. The efficiency of pretreatment was measured in terms of high-xylose and low-glucose yields, which was found most suitable at pretreatment conditions of 120°C, 120 min and 2% (v/v) acid concentration. With increased severity of pretreatment, xylose yield decreased with concomitant increase in glucose yield. The decrease in xylose yield was attributed to conversion into degradation products such as 5-hydroxylmethyl furfural (HMF) and acetic acid. The percentage of enzymatic saccharification increased with increased pretreatment severity. Saccharification of biomass pretreated at 180°C, 7 min and 0.5% (v/v) acid concentration produced the maximum glucose yield of saccharification of 352 g/kg dry matter, compared to just 97 g glucose/kg dry matter in the case of untreated biomass. The same pretreatment conditions resulted in maximum total sugar yield of pretreatment and saccharification of 459 g/kg dry matter, which was more than 67% of the total potential sugars in biomass. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21750" xmlns="http://purl.org/rss/1.0/"><title>Photoswitchable azobenzene- and stilbene-based chromophores bearing terminal nitro groups: Synthesis, thermal and photochemical properties</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21750</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Photoswitchable azobenzene- and stilbene-based chromophores bearing terminal nitro groups: Synthesis, thermal and photochemical properties</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Po-Chih Yang, Chung-Lin Lee, Wei-Chun Chen, Cheng-Yi Lin</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-10-11T09:34:04.545422-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21750</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21750</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21750</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<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 examined the effects of aromatic cores and spacer lengths of chromophore structures on photoreactivity and mesomorphic properties of a series of azobenzene- and stilbene-based chromophores bearing electron-withdrawing (<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>NO<sub>2</sub>) terminal groups caused by esterification reactions. The chromophores were composed of liquid crystalline mesophases with six or 11 methylene segments as spacers and with azobenzene (<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>N<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8fe.gif" alt="[DOUBLE BOND]"/>N<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>) and stilbene (<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>C<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8fe.gif" alt="[DOUBLE BOND]"/>C<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>) aromatic cores. The target compounds were further characterised using nuclear magnetic resonance spectroscopy, differential scanning calorimetry, polarising optical microscopy, absorption and photoluminescence spectroscopies. All of the azobenzene and stilbene derivatives with six or 11 methylene segments showed enantiotropic mesophases and revealed chiral nematic phases (cholesteric, exhibiting oily streaks textures). S6 and S11 with stilbene cores showed broader phase transition temperature ranges than A6 and A11 with azobenzene cores because of the molecular interaction enhancement of the planar stilbene structure. We investigated the effects of these photochromic compounds' structures on E/Z photoisomerisation under UV irradiation. UV irradiation caused E/Z photoisomerisation at N<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8fe.gif" alt="[DOUBLE BOND]"/>N and C<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8fe.gif" alt="[DOUBLE BOND]"/>C segments of the chromophores, leading to reversible and irreversible isomerisation respectively. These synthesised chromophores with functionally photoisomerised groups might have potential application for photoinduced alignments in liquid crystal industries. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

This study examined the effects of aromatic cores and spacer lengths of chromophore structures on photoreactivity and mesomorphic properties of a series of azobenzene- and stilbene-based chromophores bearing electron-withdrawing (<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>NO2) terminal groups caused by esterification reactions. The chromophores were composed of liquid crystalline mesophases with six or 11 methylene segments as spacers and with azobenzene (<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>N<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8fe.gif" alt="[DOUBLE BOND]"/>N<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>) and stilbene (<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>C<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8fe.gif" alt="[DOUBLE BOND]"/>C<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>) aromatic cores. The target compounds were further characterised using nuclear magnetic resonance spectroscopy, differential scanning calorimetry, polarising optical microscopy, absorption and photoluminescence spectroscopies. All of the azobenzene and stilbene derivatives with six or 11 methylene segments showed enantiotropic mesophases and revealed chiral nematic phases (cholesteric, exhibiting oily streaks textures). S6 and S11 with stilbene cores showed broader phase transition temperature ranges than A6 and A11 with azobenzene cores because of the molecular interaction enhancement of the planar stilbene structure. We investigated the effects of these photochromic compounds' structures on E/Z photoisomerisation under UV irradiation. UV irradiation caused E/Z photoisomerisation at N<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8fe.gif" alt="[DOUBLE BOND]"/>N and C<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8fe.gif" alt="[DOUBLE BOND]"/>C segments of the chromophores, leading to reversible and irreversible isomerisation respectively. These synthesised chromophores with functionally photoisomerised groups might have potential application for photoinduced alignments in liquid crystal industries. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21744" xmlns="http://purl.org/rss/1.0/"><title>Modification of the AMX membrane surface: Temperature dependence of anion exchange equilibrium</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21744</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Modification of the AMX membrane surface: Temperature dependence of anion exchange equilibrium</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Fatma Guesmi, Chiraz Hannachi, Béchir Hamrouni</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-09-24T11:20:57.410196-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21744</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21744</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21744</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separation Processes</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 order to improve the selectivity of the AMX membrane, a polyethyleneimine (PEI) layer was adsorbed on its surface. Ion exchange isotherms of (Cl<sup>−</sup>/NO<span><img alt="math image" src="http://onlinelibrary.wiley.com/store/10.1002/cjce.21744/asset/equation/tex2gif-stack-1.gif?v=1&amp;s=c99fff6e259cfc7a0a75c43f58c573de5eb6627e" class="inlineGraphic"/></span>), (Cl<sup>−</sup>/SO<span><img alt="math image" src="http://onlinelibrary.wiley.com/store/10.1002/cjce.21744/asset/equation/tex2gif-stack-2.gif?v=1&amp;s=bcc7c5aa680bbccc610a5a7e795b45f6c9fc66fd" class="inlineGraphic"/></span>) and (NO<span><img alt="math image" src="http://onlinelibrary.wiley.com/store/10.1002/cjce.21744/asset/equation/tex2gif-stack-3.gif?v=1&amp;s=d335432c926d4e66cbbdfa86e8222600ac799625" class="inlineGraphic"/></span>/SO<span><img alt="math image" src="http://onlinelibrary.wiley.com/store/10.1002/cjce.21744/asset/equation/tex2gif-stack-4.gif?v=1&amp;s=c622857260705f04d4060ddd49b13c6b372fbef6" class="inlineGraphic"/></span>), using a modified AMX membrane, were established at different temperatures (from 283 to 313 K), with a constant total concentration of 0.3 mol/L and neutral pH. The results obtained with the modified membrane in this range of temperature show that chloride was the most sorbed and the selectivity order was Cl<sup>−</sup> &gt; NO<span><img alt="math image" src="http://onlinelibrary.wiley.com/store/10.1002/cjce.21744/asset/equation/tex2gif-stack-5.gif?v=1&amp;s=a9cb61b32d7cbad1c1e68b645fde28513833094f" class="inlineGraphic"/></span> &gt; SO<span><img alt="math image" src="http://onlinelibrary.wiley.com/store/10.1002/cjce.21744/asset/equation/tex2gif-stack-6.gif?v=1&amp;s=600b663ac4592a783b290ac8373f0440fa7d970d" class="inlineGraphic"/></span>. Selectivity coefficients and thermodynamic equilibrium constants, determined for the three binary systems, increased with increasing temperature. These results were compared with those obtained with the unmodified membrane. It was observed that for the modified membrane, the selectivity towards sulphate ion decreased and the modified membrane became more selective towards monovalent anions. Ion exchange equilibrium at temperatures 283, 298 and 313 K of the studied binary systems were found to be endothermic processes. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

In order to improve the selectivity of the AMX membrane, a polyethyleneimine (PEI) layer was adsorbed on its surface. Ion exchange isotherms of (Cl−/NO 3−), (Cl−/SO 42−) and (NO 3−/SO 42−), using a modified AMX membrane, were established at different temperatures (from 283 to 313 K), with a constant total concentration of 0.3 mol/L and neutral pH. The results obtained with the modified membrane in this range of temperature show that chloride was the most sorbed and the selectivity order was Cl− &gt; NO 3− &gt; SO 42−. Selectivity coefficients and thermodynamic equilibrium constants, determined for the three binary systems, increased with increasing temperature. These results were compared with those obtained with the unmodified membrane. It was observed that for the modified membrane, the selectivity towards sulphate ion decreased and the modified membrane became more selective towards monovalent anions. Ion exchange equilibrium at temperatures 283, 298 and 313 K of the studied binary systems were found to be endothermic processes. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21743" xmlns="http://purl.org/rss/1.0/"><title>Experimental study of kerosene–water two-phase flow in a vertical pipe using hot-film and dual optical probes</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21743</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Experimental study of kerosene–water two-phase flow in a vertical pipe using hot-film and dual optical probes</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">F. A. Hamad, M. K. Khan, H. H. Bruun</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-09-24T11:20:42.31219-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21743</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21743</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21743</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena, Fluid Dynamics and Thermodynamics</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 local parameters for kerosene–water upward flow are measured in a vertical pipe of 77.8 mm inner diameter at 4200 mm from the inlet (<em>L</em>/<em>D</em> = 54) using hot-film and dual optical probes. The effect of superficial water velocity and volumetric quality on radial distribution of two-phase flow parameters is investigated. The results show the following: (i) the profiles of volume fraction and drop frequency are very similar, and increasing superficial water velocity at low volumetric qualities (&lt;18.6%) change the profile from a convex shape with peak at the pipe centreline to uniform then to concave shape with peak near the wall; (ii) the profiles of drop cut chord change from a parabolic shape with peak at centreline for low superficial water velocities to a flat shape at higher superficial water velocity, and the area-averaged drop diameter decreases with higher superficial water velocities for all volumetric qualities; (iii) velocity profiles for both phases have shapes similar to single phase flow, flatter at higher values of superficial water velocity and volumetric quality and centreline peaked at low superficial water velocities and volumetric qualities; (iv) the slip velocity decreases with radial distance having a peak at centreline and zero values near the wall; (v) introducing kerosene drops into single phase water flow results in a sharp increase in turbulent intensity, particularly at low water velocity, and the difference between the single phase and two-phase flow turbulence intensities decreases with higher superficial water velocities and (vi) the results show that interfacial area concentration increased with higher volumetric quality and higher number of bubbles thereby increases the contact area between the two phases. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

The local parameters for kerosene–water upward flow are measured in a vertical pipe of 77.8 mm inner diameter at 4200 mm from the inlet (L/D = 54) using hot-film and dual optical probes. The effect of superficial water velocity and volumetric quality on radial distribution of two-phase flow parameters is investigated. The results show the following: (i) the profiles of volume fraction and drop frequency are very similar, and increasing superficial water velocity at low volumetric qualities (&lt;18.6%) change the profile from a convex shape with peak at the pipe centreline to uniform then to concave shape with peak near the wall; (ii) the profiles of drop cut chord change from a parabolic shape with peak at centreline for low superficial water velocities to a flat shape at higher superficial water velocity, and the area-averaged drop diameter decreases with higher superficial water velocities for all volumetric qualities; (iii) velocity profiles for both phases have shapes similar to single phase flow, flatter at higher values of superficial water velocity and volumetric quality and centreline peaked at low superficial water velocities and volumetric qualities; (iv) the slip velocity decreases with radial distance having a peak at centreline and zero values near the wall; (v) introducing kerosene drops into single phase water flow results in a sharp increase in turbulent intensity, particularly at low water velocity, and the difference between the single phase and two-phase flow turbulence intensities decreases with higher superficial water velocities and (vi) the results show that interfacial area concentration increased with higher volumetric quality and higher number of bubbles thereby increases the contact area between the two phases. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21737" xmlns="http://purl.org/rss/1.0/"><title>Decomposition of 2-chlorophenol, 4-chlorophenol and 2,4,6-trichlorophenol by catalytic oxidation over cobalt and nickel impregnated SBA-15</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21737</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Decomposition of 2-chlorophenol, 4-chlorophenol and 2,4,6-trichlorophenol by catalytic oxidation over cobalt and nickel impregnated SBA-15</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Suranjana V. Mayani, Vishal J. Mayani, Sang Wook Kim</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-09-18T11:31:33.765488-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21737</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21737</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21737</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, Chemical Kinetics, and Catalysis</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 describes the use of Co(II) and Ni(II) impregnated SBA-15 as catalysts for the oxidative degradation of a few persistent chlorinated phenols in an aqueous medium: 2-chlorophenol (2-CP), 4-chlorophenol (4-CP) and 2,4,6-trichlorophenol (2,4,6-TCP). The catalysts were characterised in terms of their crystallographic features, surface topography, functional groups, thermal stability, etc. The oxidation reactions were carried out using the reaction time, concentration of chlorophenol, amount of catalyst and pH of the reaction mixture as the process variables with or without hydrogen peroxide as the chemical oxidising agent. The conversion achieved with <b>Co/SBA-15</b> for 2-CP, 4-CP and 2,4,6-TCP was respectively 84.7%, 78.4% and 64.8% with H<sub>2</sub>O<sub>2</sub> and 86.3%, 80.2% and 70.3% in the absence of H<sub>2</sub>O<sub>2</sub>. The conversion with <b>Ni/SBA-15</b> also at 353 K for 2-CP, 4-CP and 2,4,6-TCP was, respectively, 82.3%, 81.9% and 64.0% at 5 h with H<sub>2</sub>O<sub>2</sub> and 89.5%, 82.9% and 65.6% without H<sub>2</sub>O<sub>2</sub>. The reactions followed pseudo-first-order kinetics. The leachability study indicated that the catalysts release very little Co and Ni to water. Therefore, the possibility of water contamination through metal leaching was almost negligible. Oxidative degradation was confirmed by measuring the total organic carbon. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

This work describes the use of Co(II) and Ni(II) impregnated SBA-15 as catalysts for the oxidative degradation of a few persistent chlorinated phenols in an aqueous medium: 2-chlorophenol (2-CP), 4-chlorophenol (4-CP) and 2,4,6-trichlorophenol (2,4,6-TCP). The catalysts were characterised in terms of their crystallographic features, surface topography, functional groups, thermal stability, etc. The oxidation reactions were carried out using the reaction time, concentration of chlorophenol, amount of catalyst and pH of the reaction mixture as the process variables with or without hydrogen peroxide as the chemical oxidising agent. The conversion achieved with Co/SBA-15 for 2-CP, 4-CP and 2,4,6-TCP was respectively 84.7%, 78.4% and 64.8% with H2O2 and 86.3%, 80.2% and 70.3% in the absence of H2O2. The conversion with Ni/SBA-15 also at 353 K for 2-CP, 4-CP and 2,4,6-TCP was, respectively, 82.3%, 81.9% and 64.0% at 5 h with H2O2 and 89.5%, 82.9% and 65.6% without H2O2. The reactions followed pseudo-first-order kinetics. The leachability study indicated that the catalysts release very little Co and Ni to water. Therefore, the possibility of water contamination through metal leaching was almost negligible. Oxidative degradation was confirmed by measuring the total organic carbon. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21739" xmlns="http://purl.org/rss/1.0/"><title>The quality-constrained scheduling problem in plastics compounding</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21739</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">The quality-constrained scheduling problem in plastics compounding</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Abdunnaser Younes, Ali Elkamel, Michelle Leung, Costas Tzoganakis, Ali Lohi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-09-18T11:30:29.594758-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21739</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21739</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21739</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Process Systems Engineering</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>Interest is increasing in plastic compounding plants that offer tailor-made resins. Such plants produce a wide range of products in small quantities and with frequent changeovers. The underlying scheduling problem has been extensively researched; however, the concept of incorporating qualities of the finished product in the problem of plastics compounding has not been considered.</p></div>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>We express product qualities as an additional problem constraint so that the production schedule ensures product quality. The additional constraint makes this mixed integer nonlinear program (MINLP) problem more difficult to solve. Several case studies are solved to illustrate the utility of the proposed approach.</p></div>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Experiments demonstrated that qualities of the finished product can be ensured a priori if the appropriate relations are developed and integrated in the optimisation model. As well, this paper provides insight into the economic aspects of the scheduling problem under consideration. Experiments showed that none of the cost components (operation, raw material, inventory, penalty or utilities) can alone play the role of the optimisation criterion. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Interest is increasing in plastic compounding plants that offer tailor-made resins. Such plants produce a wide range of products in small quantities and with frequent changeovers. The underlying scheduling problem has been extensively researched; however, the concept of incorporating qualities of the finished product in the problem of plastics compounding has not been considered.
We express product qualities as an additional problem constraint so that the production schedule ensures product quality. The additional constraint makes this mixed integer nonlinear program (MINLP) problem more difficult to solve. Several case studies are solved to illustrate the utility of the proposed approach.
Experiments demonstrated that qualities of the finished product can be ensured a priori if the appropriate relations are developed and integrated in the optimisation model. As well, this paper provides insight into the economic aspects of the scheduling problem under consideration. Experiments showed that none of the cost components (operation, raw material, inventory, penalty or utilities) can alone play the role of the optimisation criterion. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21718" xmlns="http://purl.org/rss/1.0/"><title>Modelling and optimisation of continuous catalytic regeneration process using bee colony algorithm</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21718</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Modelling and optimisation of continuous catalytic regeneration process using bee colony algorithm</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Majid Sa'idi, Navid Mostoufi, Rahmat Sotudeh-Gharebagh</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-07-13T14:20:16.370109-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21718</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21718</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21718</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<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 continuous catalytic regeneration (CCR) reforming process optimisation leads to nonlinear programming with nonlinear quality constraints such as octane number and coke concentration on the catalytic particles. A typical CCR reforming process consists of four reactors with recycle. The reaction patterns and reactors have been mathematically modelled on a base of 12-lumped kinetics reaction network derived from literature. The bee colony optimisation (BCO) algorithm is one of the most recent and efficient swarm intelligence-based algorithms which simulates the foraging behaviour of honey bee colonies. The performance of the BCO algorithm in the process optimisation was compared with the genetic algorithm (GA). In the present work, BCO algorithm was used for optimising the CCR reforming process. The results show that the BCO algorithm reaches a better optimum point in a lower evaluation time and higher convergence rate with respect to the GA. © 2012 Canadian Society for Chemical Engineering</p></div>]]></content:encoded><description>The continuous catalytic regeneration (CCR) reforming process optimisation leads to nonlinear programming with nonlinear quality constraints such as octane number and coke concentration on the catalytic particles. A typical CCR reforming process consists of four reactors with recycle. The reaction patterns and reactors have been mathematically modelled on a base of 12-lumped kinetics reaction network derived from literature. The bee colony optimisation (BCO) algorithm is one of the most recent and efficient swarm intelligence-based algorithms which simulates the foraging behaviour of honey bee colonies. The performance of the BCO algorithm in the process optimisation was compared with the genetic algorithm (GA). In the present work, BCO algorithm was used for optimising the CCR reforming process. The results show that the BCO algorithm reaches a better optimum point in a lower evaluation time and higher convergence rate with respect to the GA. © 2012 Canadian Society for Chemical Engineering</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21632" xmlns="http://purl.org/rss/1.0/"><title>Correlation of the performance of a PEM fuel cell at different channel geometries</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21632</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Correlation of the performance of a PEM fuel cell at different channel geometries</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">I. Khazaee, M. Ghazikhani</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-12-27T16:47:02.276081-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21632</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21632</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21632</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<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 study, the performance of a proton exchange membrane fuel cell at different channel geometries is investigated experimentally. Three PEM fuel cells with different channel geometries with 25 cm<sup>2</sup> active area and Nafion 117 as membrane with 0.004 g/cm<sup>2</sup> platinum for the anode and cathode are employed as a membrane electrode assembly. Some parameters such as input oxygen temperature <span class="math"><img alt="equation image" src="http://onlinelibrary.wiley.com/store/10.1002/cjce.21632/asset/equation/tex2gif-ueqn-1.gif?v=1&amp;s=fad82a60366c5dded9186cddca813d37b412a820" class="inlineGraphic"/></span>, input hydrogen temperature <span class="math"><img alt="equation image" src="http://onlinelibrary.wiley.com/store/10.1002/cjce.21632/asset/equation/tex2gif-ueqn-2.gif?v=1&amp;s=667883b7f87b34a899380cc7fc6d4199aaa8ad0a" class="inlineGraphic"/></span>, cell temperature (45°C ≤ <em>T</em><sub>cell</sub> ≤ 65°C), input pressure (1.905 bar ≤ <em>P</em> ≤ 4.905 bar), oxygen flow rate <span class="math"><img alt="equation image" src="http://onlinelibrary.wiley.com/store/10.1002/cjce.21632/asset/equation/tex2gif-ueqn-3.gif?v=1&amp;s=824e0a244bfef82420e08d8f86aaec69f7b0bdcf" class="inlineGraphic"/></span>, hydrogen flow rate <span class="math"><img alt="equation image" src="http://onlinelibrary.wiley.com/store/10.1002/cjce.21632/asset/equation/tex2gif-ueqn-4.gif?v=1&amp;s=46f8db2742812cc34ae9ce55bffac23f86069709" class="inlineGraphic"/></span> and geometry of channels (1 ≤ <em>Z</em> ≤ 3) affect the performance of the cell. A series of experiments are carried out to investigate the influence of the above parameters on the polarisation curve under the above conditions. A semi empirical equation is offered to correlate the data for the polarisation curve. The results show that when the geometry of channel is rectangular, the performance of the cell is better than the triangular and elliptical channel. Also, results show that increase in the operating temperature and pressure can enhance the cell performance and they are compared with the results of the correlated equation and a good agreement exists. © 2011 Canadian Society for Chemical Engineering</p></div>]]></content:encoded><description>In this study, the performance of a proton exchange membrane fuel cell at different channel geometries is investigated experimentally. Three PEM fuel cells with different channel geometries with 25 cm2 active area and Nafion 117 as membrane with 0.004 g/cm2 platinum for the anode and cathode are employed as a membrane electrode assembly. Some parameters such as input oxygen temperature $(45^{{\circ} } {\rm C}\,\leq \,T_{{\rm O}_{2} } \,\leq 65^{{\circ} } {\rm C})$, input hydrogen temperature $(40^{{\circ} } {\rm C}\,\leq \,T_{{\rm H}_{2} } \,\leq \,60^{{\circ} } {\rm C})$, cell temperature (45°C ≤ Tcell ≤ 65°C), input pressure (1.905 bar ≤ P ≤ 4.905 bar), oxygen flow rate $(0.5\,{\rm L}/{\rm min}\,\leq \,{\dot {m}}_{{\rm O}_{2} } \,\leq \,0.1.3\,{\rm L}/{\rm min})$, hydrogen flow rate $(0.3\,{\rm L}/{\rm min}\,\leq \,{\dot {m}}_{{\rm H}_{2} } \,\leq \,0.9\,{\rm L}/{\rm min})$ and geometry of channels (1 ≤ Z ≤ 3) affect the performance of the cell. A series of experiments are carried out to investigate the influence of the above parameters on the polarisation curve under the above conditions. A semi empirical equation is offered to correlate the data for the polarisation curve. The results show that when the geometry of channel is rectangular, the performance of the cell is better than the triangular and elliptical channel. Also, results show that increase in the operating temperature and pressure can enhance the cell performance and they are compared with the results of the correlated equation and a good agreement exists. © 2011 Canadian Society for Chemical Engineering</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.20388" xmlns="http://purl.org/rss/1.0/"><title>Preparation and characterization of high performance (Co, Cu)/Pt/γ-Al2O3 bimetallic catalysts for oxidation of 2-propanol : Experiments and ANN modelling</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.20388</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Preparation and characterization of high performance (Co, Cu)/Pt/γ-Al2O3 bimetallic catalysts for oxidation of 2-propanol : Experiments and ANN modelling</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Darush Salari, Aligholi Niaei, Faezeh Aghazadeh, Seyed Ali Hosseini</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-04-21T14:57:15.61866-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.20388</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.20388</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.20388</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<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 catalytic oxidation of 2-propanol over a series of Pt/γ-Al<sub>2</sub>O<sub>3</sub>, Co/Pt/γ-Al<sub>2</sub>O<sub>3</sub>, and Cu/Pt/γ-Al<sub>2</sub>O<sub>3</sub> catalysts was investigated in a fixed bed reactor under atmospheric pressure and different temperatures. Among them, Co/Pt/γ-Al<sub>2</sub>O<sub>3</sub> was found to be the most promising catalyst based on activity. X-ray diffraction (XRD), scanning electron microscopy (SEM), transmission electron microscopy (TEM), X-ray photoelectron spectroscopy (XPS), and ICP-AES techniques were used to characterise a series of catalysts. The influence of reaction temperature, calcination temperature, and content of metal loading on conversion efficiency was studied. Cobalt loadings on Pt/γ-Al<sub>2</sub>O<sub>3</sub> had a great effect on catalytic activity and 3.74 wt.% Co/Pt/γ-Al<sub>2</sub>O<sub>3</sub> bimetallic catalyst at calcination temperature of 300°C was observed to be the most active. An artificial neural networks (ANN) model was developed to predict the performance of catalytic oxidation process over bimetallic catalysts based on experimental data. Levenberg–Marquardt (LM) learning algorithm was employed to train the model by using laboratory experimental data. A comparison between the predicted results of the designed ANN model and experimental data was also conducted. ANN predicted the content of metal loading is the most effective factor. The developed model can describe the catalytic oxidation over bimetallic catalysts under different conditions.</p></div><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>On a étudié l'oxydation catalytique du propan-2-ol sur une série de catalyseurs Pt/γ-Al<sub>2</sub>O<sub>3</sub>, Co/Pt/γ-Al<sub>2</sub>O<sub>3</sub> et Cu/Pt/γ-Al2O3 dans un réacteur à lit fixe sous une pression atmosphérique et différentes températures. Parmi eux, on a déterminé que le Co/Pt/γ-Al<sub>2</sub>O<sub>3</sub> était le catalyseur le plus prometteur selon l'activité. La diffraction des rayons X, la microscopie électronique à balayage (MEB), la microscopie électronique à transmission (MET), la spectroscopie de photoélectrons X et les techniques de spectrométrie d'émission ICP-AES ont été utilisées pour caractériser une série de catalyseurs. On a étudié l'influence de la température de réaction, la température de calcination et la teneur en charge de métal sur le rendement de conversion. Les charges de cobalt sur le Pt/γ-Al<sub>2</sub>O<sub>3</sub> ont eu un effet considérable sur l'activité catalytique et on a observé que le catalyseur bimétallique Co/Pt/γ-Al<sub>2</sub>O<sub>3</sub> de 3,74% d'équivalent en poids à une température de calcination de 300°C était le plus actif. Un modèle de réseaux de neurones artificiels (RNA) a été créé dans le but de prédire le rendement du processus d'oxydation catalytique sur les catalyseurs bimétalliques fondé sur les données expérimentales. L'algorithme d'apprentissage Levenberg–Marquardt (LM) a été utilisé pour former le modèle au moyen de données expérimentales de laboratoire. On a également procédé à une comparaison entre les résultats prédits du modèle de RNA conçu et les données expérimentales. Les RNA ont prédit que la teneur en charge de métal constitue le facteur le plus efficace. Le modèle créé peut décrire l'oxydation catalytique sur les catalyseurs bimétalliques dans différentes conditions. © 2011 Canadian Society for Chemical Engineering</p></div>]]></content:encoded><description>The catalytic oxidation of 2-propanol over a series of Pt/γ-Al2O3, Co/Pt/γ-Al2O3, and Cu/Pt/γ-Al2O3 catalysts was investigated in a fixed bed reactor under atmospheric pressure and different temperatures. Among them, Co/Pt/γ-Al2O3 was found to be the most promising catalyst based on activity. X-ray diffraction (XRD), scanning electron microscopy (SEM), transmission electron microscopy (TEM), X-ray photoelectron spectroscopy (XPS), and ICP-AES techniques were used to characterise a series of catalysts. The influence of reaction temperature, calcination temperature, and content of metal loading on conversion efficiency was studied. Cobalt loadings on Pt/γ-Al2O3 had a great effect on catalytic activity and 3.74 wt.% Co/Pt/γ-Al2O3 bimetallic catalyst at calcination temperature of 300°C was observed to be the most active. An artificial neural networks (ANN) model was developed to predict the performance of catalytic oxidation process over bimetallic catalysts based on experimental data. Levenberg–Marquardt (LM) learning algorithm was employed to train the model by using laboratory experimental data. A comparison between the predicted results of the designed ANN model and experimental data was also conducted. ANN predicted the content of metal loading is the most effective factor. The developed model can describe the catalytic oxidation over bimetallic catalysts under different conditions.On a étudié l'oxydation catalytique du propan-2-ol sur une série de catalyseurs Pt/γ-Al2O3, Co/Pt/γ-Al2O3 et Cu/Pt/γ-Al2O3 dans un réacteur à lit fixe sous une pression atmosphérique et différentes températures. Parmi eux, on a déterminé que le Co/Pt/γ-Al2O3 était le catalyseur le plus prometteur selon l'activité. La diffraction des rayons X, la microscopie électronique à balayage (MEB), la microscopie électronique à transmission (MET), la spectroscopie de photoélectrons X et les techniques de spectrométrie d'émission ICP-AES ont été utilisées pour caractériser une série de catalyseurs. On a étudié l'influence de la température de réaction, la température de calcination et la teneur en charge de métal sur le rendement de conversion. Les charges de cobalt sur le Pt/γ-Al2O3 ont eu un effet considérable sur l'activité catalytique et on a observé que le catalyseur bimétallique Co/Pt/γ-Al2O3 de 3,74% d'équivalent en poids à une température de calcination de 300°C était le plus actif. Un modèle de réseaux de neurones artificiels (RNA) a été créé dans le but de prédire le rendement du processus d'oxydation catalytique sur les catalyseurs bimétalliques fondé sur les données expérimentales. L'algorithme d'apprentissage Levenberg–Marquardt (LM) a été utilisé pour former le modèle au moyen de données expérimentales de laboratoire. On a également procédé à une comparaison entre les résultats prédits du modèle de RNA conçu et les données expérimentales. Les RNA ont prédit que la teneur en charge de métal constitue le facteur le plus efficace. Le modèle créé peut décrire l'oxydation catalytique sur les catalyseurs bimétalliques dans différentes conditions. © 2011 Canadian Society for Chemical Engineering</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.20476" xmlns="http://purl.org/rss/1.0/"><title>Retracted: Carbonaceous degradation of endocrine disruption chemicals (EDCs) using ozonolysis—studied with sparger effect for minimum ozone consumption</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.20476</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Retracted: Carbonaceous degradation of endocrine disruption chemicals (EDCs) using ozonolysis—studied with sparger effect for minimum ozone consumption</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. S. Islam, A. Blondy, K. L. Yeung, M. A. A. S. Choudhury, A. Julbe, A. Ayral, S. Heng, J. C. Schrotter</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2011-02-09T16:49:02.356568-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.20476</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.20476</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.20476</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Retraction</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 following article from the Canadian Journal of Chemical Engineering, “Carbonaceous degradation of endocrine disruption chemicals (EDCs) using ozonolysis - studied with sparger effect for minimum ozone consumption” by M. S. Islam, et al., published online on February 9, 2011 in Wiley Online Library (wileyonlinelibrary.com), has been retracted by agreement between the authors, the journal Editor-in-Chief, Joao B. P. Soares, and Wiley Periodicals, Inc. The retraction has been agreed because the co-authors did not approve the inclusion of their names in the article.</p></div>]]></content:encoded><description>The following article from the Canadian Journal of Chemical Engineering, “Carbonaceous degradation of endocrine disruption chemicals (EDCs) using ozonolysis - studied with sparger effect for minimum ozone consumption” by M. S. Islam, et al., published online on February 9, 2011 in Wiley Online Library (wileyonlinelibrary.com), has been retracted by agreement between the authors, the journal Editor-in-Chief, Joao B. P. Soares, and Wiley Periodicals, Inc. The retraction has been agreed because the co-authors did not approve the inclusion of their names in the article.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21813" xmlns="http://purl.org/rss/1.0/"><title>Semicontinuous separation of dimethyl ether (DME) produced from biomass</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21813</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Semicontinuous separation of dimethyl ether (DME) produced from biomass</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Alicia Pascall, Thomas A. Adams</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-26T09:18:06.062095-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21813</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21813</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21813</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Special Series</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1001</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1021</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 ternary semicontinuous system for the separation of bio-dimethyl ether from methanol and water is presented. The performance of eight potential control configurations, including the application of temperature inferential control, is evaluated. Dynamic simulations of the semicontinuous system and associated control scheme demonstrate that the temperature inferential control configuration is effective in achieving the separation objectives while remaining within operational limits. The semicontinuous system using the inferential temperature control scheme is simulated and shown to be economically preferable to the traditional continuous process for a range of production rates. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

A ternary semicontinuous system for the separation of bio-dimethyl ether from methanol and water is presented. The performance of eight potential control configurations, including the application of temperature inferential control, is evaluated. Dynamic simulations of the semicontinuous system and associated control scheme demonstrate that the temperature inferential control configuration is effective in achieving the separation objectives while remaining within operational limits. The semicontinuous system using the inferential temperature control scheme is simulated and shown to be economically preferable to the traditional continuous process for a range of production rates. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21734" xmlns="http://purl.org/rss/1.0/"><title>Cadmium(II) biosorption from aqueous solutions using Hydrilla verticillata</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21734</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Cadmium(II) biosorption from aqueous solutions using Hydrilla verticillata</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Guo-Xin Li, Chang-Zhou Yan, Dan-Dan Zhang, Chao Zhao, Guo-Yuan Chen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-09-24T11:17:41.604427-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21734</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21734</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21734</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1022</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1030</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 kinetics and equilibrium of cadmium biosorption from aqueous solutions were investigated using fresh tissues of <em>Hydrilla verticillata</em>. The biosorptive characteristics of cadmium ions were studied with respect to well-established effective parameters, including pH, temperature and contact time. The biosorptive capacity of <em>H. verticillata</em> for cadmium increased with increasing pH. In addition, the resulting isotherms were well-described by Langmuir and extended Langmuir models (<em>R</em><sup>2</sup> = 0.9794–0.9957 and 0.9880, respectively). The comparison between calculated and experimental <em>q</em><sub>e</sub> values showed that the extended Langmuir model had a better simulation for the cadmium biosorption by <em>H. verticillata</em> than the Langmuir isotherm model. The equilibrium biosorption data at a constant temperature were well-interpreted by the Langmuir model. The maximum biosorptive capacity increased from 33.54 to 37.46 mg/g when the solution temperature was increased from 278 to 298 K. Other various thermodynamic parameters were also estimated. Biosorptive equilibrium was established within approximately 20 min. Moreover, the pseudo-second-order equation was more appropriate in predicting biosorptive capacity than the pseudo-first-order equation. In practical viewpoints, the abundant and inexpensive plant biomass <em>H. verticillata</em> can be used as an effective and environmentally friendly biosorbent for the detoxification of cadmium from aqueous solutions. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

The kinetics and equilibrium of cadmium biosorption from aqueous solutions were investigated using fresh tissues of Hydrilla verticillata. The biosorptive characteristics of cadmium ions were studied with respect to well-established effective parameters, including pH, temperature and contact time. The biosorptive capacity of H. verticillata for cadmium increased with increasing pH. In addition, the resulting isotherms were well-described by Langmuir and extended Langmuir models (R2 = 0.9794–0.9957 and 0.9880, respectively). The comparison between calculated and experimental qe values showed that the extended Langmuir model had a better simulation for the cadmium biosorption by H. verticillata than the Langmuir isotherm model. The equilibrium biosorption data at a constant temperature were well-interpreted by the Langmuir model. The maximum biosorptive capacity increased from 33.54 to 37.46 mg/g when the solution temperature was increased from 278 to 298 K. Other various thermodynamic parameters were also estimated. Biosorptive equilibrium was established within approximately 20 min. Moreover, the pseudo-second-order equation was more appropriate in predicting biosorptive capacity than the pseudo-first-order equation. In practical viewpoints, the abundant and inexpensive plant biomass H. verticillata can be used as an effective and environmentally friendly biosorbent for the detoxification of cadmium from aqueous solutions. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21756" xmlns="http://purl.org/rss/1.0/"><title>Separation of CO2 and CH4 on CaX zeolite for use in Landfill gas separation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21756</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Separation of CO2 and CH4 on CaX zeolite for use in Landfill gas separation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sarah Oddy, Jessica Poupore, F. Handan Tezel</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-19T07:34:58.032037-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21756</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21756</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21756</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1031</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1039</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 study, adsorption separation of main components of landfill gas, methane (CH<sub>4</sub>) and carbon dioxide (CO<sub>2</sub>) was carried out. Henry's law constants, limiting heat of adsorption values, pure and binary isotherms for CO<sub>2</sub> and CH<sub>4</sub> were determined for CaX zeolite adsorbent. Pure isotherm data were compared to those for NaX zeolite from previous studies. The CO<sub>2</sub> adsorption capacity of CaX was greater than that of NaX; however, NaX's separation factor was higher. The heat of adsorption for CO<sub>2</sub> for CaX was higher than those for NaX. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

In this study, adsorption separation of main components of landfill gas, methane (CH4) and carbon dioxide (CO2) was carried out. Henry's law constants, limiting heat of adsorption values, pure and binary isotherms for CO2 and CH4 were determined for CaX zeolite adsorbent. Pure isotherm data were compared to those for NaX zeolite from previous studies. The CO2 adsorption capacity of CaX was greater than that of NaX; however, NaX's separation factor was higher. The heat of adsorption for CO2 for CaX was higher than those for NaX. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21817" xmlns="http://purl.org/rss/1.0/"><title>Effect of torrefaction on the density and volume changes of coarse biomass particles</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21817</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of torrefaction on the density and volume changes of coarse biomass particles</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Prabir Basu, Shailendra Rao, Bishnu Acharya, Alok Dhungana</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-26T09:18:18.321382-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21817</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21817</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21817</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1040</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1044</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 provides preliminary data on the effect of torrefaction on the apparent density of biomass. It also examines how the shape of wood is affected by torrefaction. Experiments conducted on cylinders of poplar wood showed that torrefaction reduced both density and volume of the wood, and the extent of reduction increased with increase in severity of torrefaction. The shape of the wood appears to have some effect on the extent of density change. The shrinkage in radial direction was 3–4%, while reduction in longitudinal direction was 6.5–8.8%. The mass yield decreased with torrefaction severity. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

This work provides preliminary data on the effect of torrefaction on the apparent density of biomass. It also examines how the shape of wood is affected by torrefaction. Experiments conducted on cylinders of poplar wood showed that torrefaction reduced both density and volume of the wood, and the extent of reduction increased with increase in severity of torrefaction. The shape of the wood appears to have some effect on the extent of density change. The shrinkage in radial direction was 3–4%, while reduction in longitudinal direction was 6.5–8.8%. The mass yield decreased with torrefaction severity. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21729" xmlns="http://purl.org/rss/1.0/"><title>Aerobic granulation for wastewater bioremediation: A review</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21729</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Aerobic granulation for wastewater bioremediation: A review</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mohammad Zain Khan, Pijush Kanti Mondal, Suhail Sabir</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-10-11T09:33:51.542808-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21729</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21729</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21729</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1045</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1058</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>Rapid industrialisation and urbanisation releases numerous toxic compounds into natural water bodies, polluting these pristine fresh water resources. This is a subject of great concern, and the attention of environmentalists around the world has been increased towards this problem in recent years. Several techniques have been proposed for efficient wastewater treatment, most of them presenting some limitations, such as poor capacity, the generation of waste products, incomplete mineralisation and a high operating cost. Currently, aerobic granulation treatments are considered to be the most effective and economic alternative. Aerobic granulation is a process of microbial self-immobilisation that results into a cell-structured shape, characterised by dense biomass. Aerobic granules have a number of advantages over conventional bioflocs, such as a round and compact structure, good settling ability, high biomass retention and the ability to withstand high organic loading rates. Aerobic granulation technology has been demonstrated to be useful for a wide variety of wastewaters, including industrial, nutrient-rich and toxic. This paper presents a state-of-the-art review of effective aerobic granulation technology for wastewater treatment selected from the point-of-view of basic concepts of aerobic granulation, characterisation and factors that affect aerobic granulation, demonstrating the effectiveness of the cell-immobilisation (aerobic granulation) technique. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Rapid industrialisation and urbanisation releases numerous toxic compounds into natural water bodies, polluting these pristine fresh water resources. This is a subject of great concern, and the attention of environmentalists around the world has been increased towards this problem in recent years. Several techniques have been proposed for efficient wastewater treatment, most of them presenting some limitations, such as poor capacity, the generation of waste products, incomplete mineralisation and a high operating cost. Currently, aerobic granulation treatments are considered to be the most effective and economic alternative. Aerobic granulation is a process of microbial self-immobilisation that results into a cell-structured shape, characterised by dense biomass. Aerobic granules have a number of advantages over conventional bioflocs, such as a round and compact structure, good settling ability, high biomass retention and the ability to withstand high organic loading rates. Aerobic granulation technology has been demonstrated to be useful for a wide variety of wastewaters, including industrial, nutrient-rich and toxic. This paper presents a state-of-the-art review of effective aerobic granulation technology for wastewater treatment selected from the point-of-view of basic concepts of aerobic granulation, characterisation and factors that affect aerobic granulation, demonstrating the effectiveness of the cell-immobilisation (aerobic granulation) technique. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21725" xmlns="http://purl.org/rss/1.0/"><title>Liquid degassing using mono-dispersed and poly-dispersed micron droplets</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21725</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Liquid degassing using mono-dispersed and poly-dispersed micron droplets</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yiming Ji, Zhenghe Xu, Zhongchao Tan</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-08-08T09:54:09.838008-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21725</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21725</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21725</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1059</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1068</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>Liquid degassing using mono-dispersed and poly-dispersed micron droplets (148.6 and 264.8 µm) falling in an inert gas was studied experimentally and analytically in a laboratory setting. The system using poly-dispersed droplets revealed an upper degassing limit of 93% when the inert gas to liquid flow ratio was above 15 and a fog-type nozzle was used. Linear correlations of the Sherwood number to the Peclet number were derived for both systems of medium Reynolds numbers (10–100). The correlation for the mono-dispersed droplets agreed well with the steady state mass transfer correlations that are available in literature, especially at small Peclet number situations. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Liquid degassing using mono-dispersed and poly-dispersed micron droplets (148.6 and 264.8 µm) falling in an inert gas was studied experimentally and analytically in a laboratory setting. The system using poly-dispersed droplets revealed an upper degassing limit of 93% when the inert gas to liquid flow ratio was above 15 and a fog-type nozzle was used. Linear correlations of the Sherwood number to the Peclet number were derived for both systems of medium Reynolds numbers (10–100). The correlation for the mono-dispersed droplets agreed well with the steady state mass transfer correlations that are available in literature, especially at small Peclet number situations. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21717" xmlns="http://purl.org/rss/1.0/"><title>Reductions in cod and acute toxicity of wastewater generated from refined cotton production using activated carbon fibre (ACF)</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21717</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Reductions in cod and acute toxicity of wastewater generated from refined cotton production using activated carbon fibre (ACF)</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Xu Zhao, Quanlin Zhao, Qingqiang Meng, Wei Xia, Zhengfang Ye</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-08-17T09:30:50.021562-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21717</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21717</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21717</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1069</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1076</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>Activated carbon fibre is investigated for adsorption of organic pollutants from wastewater generated from refined cotton production. UV–Vis spectroscopy and FTIR are used to evaluate the chemical changes. Results indicate that the main organic components of refined cotton production wastewater are guaiacyl (G-) and hydroxyphenyl (H-) lignin. It is found that 85% of COD can be removed at 40°C with ACF dosage of 90 g L<sup>−1</sup>. The adsorption process is described by the Redlich–Peterson isotherm model. The kinetic data follows a pseudo-second-order equation. Over 99% of acute toxicity for Refined Cotton Production (RCP) wastewater has been reduced after adsorption using ACF. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Activated carbon fibre is investigated for adsorption of organic pollutants from wastewater generated from refined cotton production. UV–Vis spectroscopy and FTIR are used to evaluate the chemical changes. Results indicate that the main organic components of refined cotton production wastewater are guaiacyl (G-) and hydroxyphenyl (H-) lignin. It is found that 85% of COD can be removed at 40°C with ACF dosage of 90 g L−1. The adsorption process is described by the Redlich–Peterson isotherm model. The kinetic data follows a pseudo-second-order equation. Over 99% of acute toxicity for Refined Cotton Production (RCP) wastewater has been reduced after adsorption using ACF. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21720" xmlns="http://purl.org/rss/1.0/"><title>An optimisation approach for increasing the profit of a commercial VGO hydrocracking process</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21720</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">An optimisation approach for increasing the profit of a commercial VGO hydrocracking process</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sepehr Sadighi, Arshad Ahmad</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-07-25T13:57:05.052429-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21720</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21720</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21720</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1077</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1091</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 paper, an optimisation approach is proposed to increase the profit of a commercial hydrocracking unit called Isomax. To represent the system, a full-lump kinetic model incorporating the flow rate of fresh vacuum gas oil (VGO), bed temperatures, recycle flow rate and the catalyst life is developed. This model is capable of predicting the yield of all products, and it improves with respect to the previous works by considering LPG and light gases, fresh VGO and recycle streams as separate lumps. After developing and validating the model, the profit function of the plant, including the value of the products, fresh feed and hydrogen, as well as energy expenses, is optimised by manipulating the bed temperatures, flow rate of fresh VGO and combined feed ratio (CFR) whilst all process limitations and operating constraints are taken into account. During two years of study and considering all mechanical and operational constraints, the results confirm that the decision variables, generated by the optimisation package, can increase the gross profit of the Isomax process to about 8.17%, which is equal to $5.6 million of net profit annually. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

In this paper, an optimisation approach is proposed to increase the profit of a commercial hydrocracking unit called Isomax. To represent the system, a full-lump kinetic model incorporating the flow rate of fresh vacuum gas oil (VGO), bed temperatures, recycle flow rate and the catalyst life is developed. This model is capable of predicting the yield of all products, and it improves with respect to the previous works by considering LPG and light gases, fresh VGO and recycle streams as separate lumps. After developing and validating the model, the profit function of the plant, including the value of the products, fresh feed and hydrogen, as well as energy expenses, is optimised by manipulating the bed temperatures, flow rate of fresh VGO and combined feed ratio (CFR) whilst all process limitations and operating constraints are taken into account. During two years of study and considering all mechanical and operational constraints, the results confirm that the decision variables, generated by the optimisation package, can increase the gross profit of the Isomax process to about 8.17%, which is equal to $5.6 million of net profit annually. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21721" xmlns="http://purl.org/rss/1.0/"><title>Modelling of multicomponent gas separation with asymmetric hollow fibre membranes—methane enrichment from biogas</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21721</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Modelling of multicomponent gas separation with asymmetric hollow fibre membranes—methane enrichment from biogas</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Prodip K. Kundu, Amit Chakma, Xianshe Feng</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-08-07T12:00:54.016911-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21721</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21721</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21721</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1092</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1102</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 mathematical model for the dynamic performance of gas separation with high flux, asymmetric hollow fibre membranes was developed considering the permeate pressure build-up inside the fibre bore and cross flow pattern with respect to the membrane skin. The solution technique provides reliable examination of pressure and concentration profiles along the permeator length (both residue/permeate streams) with minimal effort. The proposed simulation model and scheme were validated with experimental data of gas separation from literature. The model and solution technique were applied to investigate dynamic performance of several membrane module configurations for methane recovery from biogas (landfill gas or digester gas), considering biogas as a mixture of CO<sub>2</sub>, N<sub>2</sub> and CH<sub>4</sub>. Recycle ratio plays a crucial role, and optimum recycle ratio vital for the retentate recycle to permeate and permeate recycle to feed operation was found. From the concept of two recycle operations, complexities involved in the design and operation of continuous membrane column were simplified. Membrane permselectivity required for a targeted separation to produce pipeline quality natural gas by methane-selective or nitrogen-selective membranes was calculated. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

A mathematical model for the dynamic performance of gas separation with high flux, asymmetric hollow fibre membranes was developed considering the permeate pressure build-up inside the fibre bore and cross flow pattern with respect to the membrane skin. The solution technique provides reliable examination of pressure and concentration profiles along the permeator length (both residue/permeate streams) with minimal effort. The proposed simulation model and scheme were validated with experimental data of gas separation from literature. The model and solution technique were applied to investigate dynamic performance of several membrane module configurations for methane recovery from biogas (landfill gas or digester gas), considering biogas as a mixture of CO2, N2 and CH4. Recycle ratio plays a crucial role, and optimum recycle ratio vital for the retentate recycle to permeate and permeate recycle to feed operation was found. From the concept of two recycle operations, complexities involved in the design and operation of continuous membrane column were simplified. Membrane permselectivity required for a targeted separation to produce pipeline quality natural gas by methane-selective or nitrogen-selective membranes was calculated. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21735" xmlns="http://purl.org/rss/1.0/"><title>Design of a multivariable internal model controller based on singular value decomposition</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21735</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Design of a multivariable internal model controller based on singular value decomposition</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Qi-bing Jin, Liang Zhao, Feng Hao, Si-wen Liu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-09-07T07:04:03.292279-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21735</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21735</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21735</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1103</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1114</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 article, a novel internal model control (IMC) approach based on singular value decomposition (SVD) is proposed for the control of multiple-input–multiple-output (MIMO) systems with multiple time delays. This approach achieves decoupling using a compensation term and improves the robustness using SVD in the inverse of the steady-state gain matrix of process. Meanwhile, a novel filter is designed for decoupling and fast response speed of multivariable systems with multiple delays. The design of the controller can be extended to non-square systems where there are more inputs than outputs. Examples are included to illustrate the effectiveness of the method. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

In this article, a novel internal model control (IMC) approach based on singular value decomposition (SVD) is proposed for the control of multiple-input–multiple-output (MIMO) systems with multiple time delays. This approach achieves decoupling using a compensation term and improves the robustness using SVD in the inverse of the steady-state gain matrix of process. Meanwhile, a novel filter is designed for decoupling and fast response speed of multivariable systems with multiple delays. The design of the controller can be extended to non-square systems where there are more inputs than outputs. Examples are included to illustrate the effectiveness of the method. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21803" xmlns="http://purl.org/rss/1.0/"><title>Modelling of penetration of horizontal supersonic nozzles in high temperature fluidised beds</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21803</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Modelling of penetration of horizontal supersonic nozzles in high temperature fluidised beds</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Feng Li, Cedric Briens, Franco Berruti, Jennifer McMillan</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-30T11:11:20.473942-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21803</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21803</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21803</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1115</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1130</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>Supersonic nozzles have been applied in various jet-induced fluidised bed attrition processes such as jet milling and Fluid Coking. In jet-induced particle attrition, the penetration length into the bed of the jet issuing from the supersonic nozzle is a critical property that affects the attrition mechanisms. A numerical model was developed to predict the penetration length of jets issuing from a horizontal supersonic nozzle in high temperature fluidised beds, based on an Eulerian–Eulerian multiphase model and Granular kinetic theory. The predicted jet penetration lengths are in very good agreement with the experimental data and the predictions of Li's empirical correlation [Li, “Penetration of High Velocity Horizontal Gas Jets Into a Fluidized Bed at High Temperature”, in <em>Fluidization XIII</em>, S. D. Kim, Y. Kang, J. K. Lee, Y. C. Seo, Eds., Gyeong-ju, Korea <b>2010</b>; <em>Engineering Conferences International</em>, Gyeong-ju, Korea <b>2010</b>, pp. 893–900.]. The simulation results have also demonstrated that the fluidisation velocity and bed temperature have little influence on jet penetration length. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Supersonic nozzles have been applied in various jet-induced fluidised bed attrition processes such as jet milling and Fluid Coking. In jet-induced particle attrition, the penetration length into the bed of the jet issuing from the supersonic nozzle is a critical property that affects the attrition mechanisms. A numerical model was developed to predict the penetration length of jets issuing from a horizontal supersonic nozzle in high temperature fluidised beds, based on an Eulerian–Eulerian multiphase model and Granular kinetic theory. The predicted jet penetration lengths are in very good agreement with the experimental data and the predictions of Li's empirical correlation [Li, “Penetration of High Velocity Horizontal Gas Jets Into a Fluidized Bed at High Temperature”, in Fluidization XIII, S. D. Kim, Y. Kang, J. K. Lee, Y. C. Seo, Eds., Gyeong-ju, Korea 2010; Engineering Conferences International, Gyeong-ju, Korea 2010, pp. 893–900.]. The simulation results have also demonstrated that the fluidisation velocity and bed temperature have little influence on jet penetration length. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21742" xmlns="http://purl.org/rss/1.0/"><title>Hydrolysis of imidazole and 2-chloropyridine under subcritical and supercritical water conditions</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21742</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Hydrolysis of imidazole and 2-chloropyridine under subcritical and supercritical water conditions</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Carmen Barrera-Ventura, Dolors Salvatierra, Francesc Giralt, Jaume Giralt</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-09-24T11:21:07.55982-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21742</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21742</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21742</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1131</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1139</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>Imidazole and 2-chloropyridine were used as model molecules to investigate the acid hydrolysis kinetics of agrochemicals in high-temperature water in a batch reactor system at 28 MPa. Pseudo-first-order hydrolysis reaction rate constants for the acid hydrolysis of Imidazole and 2-chloropyridine were determined in the temperature ranges 200–600 and 400–575°C, respectively, at 28 MPa. Rate constants for both compounds increased with temperature with a local maximum observed at around 400°C due to changes in the physical properties of the solvent. Imidazole and 2-chloropyridine conversions of 0.95 and 0.99999 were respectively attained at the highest temperature after 30 min of reaction. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Imidazole and 2-chloropyridine were used as model molecules to investigate the acid hydrolysis kinetics of agrochemicals in high-temperature water in a batch reactor system at 28 MPa. Pseudo-first-order hydrolysis reaction rate constants for the acid hydrolysis of Imidazole and 2-chloropyridine were determined in the temperature ranges 200–600 and 400–575°C, respectively, at 28 MPa. Rate constants for both compounds increased with temperature with a local maximum observed at around 400°C due to changes in the physical properties of the solvent. Imidazole and 2-chloropyridine conversions of 0.95 and 0.99999 were respectively attained at the highest temperature after 30 min of reaction. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21712" xmlns="http://purl.org/rss/1.0/"><title>Coupled transport of Pb2+ through tri-n-octylamine-xylene-polypropylene supported liquid membranes</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21712</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Coupled transport of Pb2+ through tri-n-octylamine-xylene-polypropylene supported liquid membranes</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Saeed ur Rehman, Gul Akhtar, M. Ashraf Chaudry</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-07-13T14:26:46.347809-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21712</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21712</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21712</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1140</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1152</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>Transport of Pb<sup>2+</sup> was carried from acidic solution into alkaline stripping phase through tri-<em>n</em>-octylamine-xylene-polypropylene supported liquid membrane. The transport of Pb<sup>2+</sup> through the membrane was studied by varying the concentration of Pb<sup>2+</sup> and HNO<sub>3</sub> in feed solution, NaOH concentration in strip solution and TOA concentration in membrane phase. The flux data obtained has been used to study the stoichiometry of complex Pb(NO<sub>3</sub>)<sub><em>n</em>+2</sub>(HNR<sub>3</sub>)<sub><em>n</em></sub>. The supported liquid membrane (SLM) has been found stable for 10 runs with 24 h between each run. This SLM has been used effectively to extract lead ions along with chromium, copper and zinc ions from aqueous acidic leached solution of paint and industrial effluents. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Transport of Pb2+ was carried from acidic solution into alkaline stripping phase through tri-n-octylamine-xylene-polypropylene supported liquid membrane. The transport of Pb2+ through the membrane was studied by varying the concentration of Pb2+ and HNO3 in feed solution, NaOH concentration in strip solution and TOA concentration in membrane phase. The flux data obtained has been used to study the stoichiometry of complex Pb(NO3)n+2(HNR3)n. The supported liquid membrane (SLM) has been found stable for 10 runs with 24 h between each run. This SLM has been used effectively to extract lead ions along with chromium, copper and zinc ions from aqueous acidic leached solution of paint and industrial effluents. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21751" xmlns="http://purl.org/rss/1.0/"><title>Solvent screening for non-aqueous extraction of Alberta oil sands</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21751</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Solvent screening for non-aqueous extraction of Alberta oil sands</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hossein Nikakhtari, Lisa Vagi, Phillip Choi, Qi Liu, Murray R. Gray</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-10-30T14:56:31.692595-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21751</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21751</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21751</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1153</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1160</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>Non-aqueous extraction of bitumen from oil sands has the potential to reduce fresh water demand of the extraction process and eliminate tailings ponds. In this study, different light hydrocarbon solvents, including aromatics, cycloalkanes, biologically derived solvents and mixtures of solvents were compared for extraction of bitumen from Alberta oil sands at room temperature and ambient pressure. The solvents are compared based on bitumen recovery, the amount of residual solvent in the extracted oil sands tailings and the content of fine solids in the extracted bitumen. The extraction experiments were carried out in a multistage process with agitation in rotary mixers and vibration sieving. The oil sands tailings were dried under ambient conditions, and their residual solvent contents were measured by a purge and trap system followed by gas chromatography. The elemental compositions of the extraction tailings were measured to calculate bitumen recovery. Supernatants from the extraction tests were centrifuged to separate and measure the contents of fine solid particles. Except for limonene and isoprene, the tested solvents showed good bitumen recoveries of around 95%. The solvent drying rates and residual solvent contents in the extracted oil sands tailings correlated to solvent vapour pressure. The contents of fine solids in the extracted bitumen (supernatant) were below 2.9% for all solvents except <em>n</em>-heptane-rich ones. Based on these findings, cyclohexane is the best candidate solvent for bitumen extraction, with 94.4% bitumen recovery, 5 mg of residual solvent per kilogram of extraction tailings and 1.4 wt% fine solids in the recovered bitumen. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Non-aqueous extraction of bitumen from oil sands has the potential to reduce fresh water demand of the extraction process and eliminate tailings ponds. In this study, different light hydrocarbon solvents, including aromatics, cycloalkanes, biologically derived solvents and mixtures of solvents were compared for extraction of bitumen from Alberta oil sands at room temperature and ambient pressure. The solvents are compared based on bitumen recovery, the amount of residual solvent in the extracted oil sands tailings and the content of fine solids in the extracted bitumen. The extraction experiments were carried out in a multistage process with agitation in rotary mixers and vibration sieving. The oil sands tailings were dried under ambient conditions, and their residual solvent contents were measured by a purge and trap system followed by gas chromatography. The elemental compositions of the extraction tailings were measured to calculate bitumen recovery. Supernatants from the extraction tests were centrifuged to separate and measure the contents of fine solid particles. Except for limonene and isoprene, the tested solvents showed good bitumen recoveries of around 95%. The solvent drying rates and residual solvent contents in the extracted oil sands tailings correlated to solvent vapour pressure. The contents of fine solids in the extracted bitumen (supernatant) were below 2.9% for all solvents except n-heptane-rich ones. Based on these findings, cyclohexane is the best candidate solvent for bitumen extraction, with 94.4% bitumen recovery, 5 mg of residual solvent per kilogram of extraction tailings and 1.4 wt% fine solids in the recovered bitumen. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21807" xmlns="http://purl.org/rss/1.0/"><title>Enhancement of the liquid feed distribution in gas solid fluidised beds by non-mechanically induced nozzle pulsations</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21807</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Enhancement of the liquid feed distribution in gas solid fluidised beds by non-mechanically induced nozzle pulsations</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Rana Sabouni, Cedric Briens, Franco Berruti</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-26T09:18:02.076493-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21807</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21807</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21807</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1161</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1167</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 non-mechanically induced nozzle pulsations was investigated in the current work, and it was found that appropriately tailored spray nozzles pulsations resulted in the dramatic improvement of the liquid feed spray distribution on particles of a fluidised bed. Non-mechanically induced pulsations were imposed on the liquid spray, using liquid and gas circuits that favour the development of beneficial pulsations. The resulting effect on liquid dispersion on the fluidised bed particles was determined with a conductance method. © 2013 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

The effect of non-mechanically induced nozzle pulsations was investigated in the current work, and it was found that appropriately tailored spray nozzles pulsations resulted in the dramatic improvement of the liquid feed spray distribution on particles of a fluidised bed. Non-mechanically induced pulsations were imposed on the liquid spray, using liquid and gas circuits that favour the development of beneficial pulsations. The resulting effect on liquid dispersion on the fluidised bed particles was determined with a conductance method. © 2013 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21752" xmlns="http://purl.org/rss/1.0/"><title>New algebraic expressions for thermodiffusion in binary n-alkane mixtures</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21752</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">New algebraic expressions for thermodiffusion in binary n-alkane mixtures</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Seshasai Srinivasan, M. Ziad Saghir</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-11-01T13:13:05.676189-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21752</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21752</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21752</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1168</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1174</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>Following a detailed analysis of the experimental data on thermodiffusion coefficients of numerous binary hydrocarbon mixtures from over 90 experiments, four new algebraic expressions are proposed. As per these formulations, the thermodiffusion coefficient of binary <em>n</em>-alkane mixtures can be expressed as a function of the chemical composition of the mixture and the mixture properties such as density and viscosity. Detailed experimental validation is presented using four <em>n</em>-alkane series containing a wide range of combinations of <em>n</em>-alkanes. Additionally, comparison with recently proposed neural network model and a model based on the principles of non-equilibrium thermodynamics is also presented. It has been found that the proposed algebraic models are simple in formulations, are evaluated with least computational effort and yet have a very high accuracy in predicting the thermodiffusion coefficients. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Following a detailed analysis of the experimental data on thermodiffusion coefficients of numerous binary hydrocarbon mixtures from over 90 experiments, four new algebraic expressions are proposed. As per these formulations, the thermodiffusion coefficient of binary n-alkane mixtures can be expressed as a function of the chemical composition of the mixture and the mixture properties such as density and viscosity. Detailed experimental validation is presented using four n-alkane series containing a wide range of combinations of n-alkanes. Additionally, comparison with recently proposed neural network model and a model based on the principles of non-equilibrium thermodynamics is also presented. It has been found that the proposed algebraic models are simple in formulations, are evaluated with least computational effort and yet have a very high accuracy in predicting the thermodiffusion coefficients. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21740" xmlns="http://purl.org/rss/1.0/"><title>Application of radioactive particle tracking to indicate shed fouling in the stripper section of a fluid coker</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21740</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Application of radioactive particle tracking to indicate shed fouling in the stripper section of a fluid coker</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Francisco J. Sanchez, Mikhail Granovskiy</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-09-24T11:06:49.843623-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21740</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21740</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21740</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1175</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1182</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 stripper section of a fluid-coker consists of a system of baffles (sheds) that enhances the removal efficiency of entrained and adsorbed hydrocarbons from the fluidised coke-particles. If the particles contain a thin liquid film layer of heavy hydrocarbons, making them excessively ‘wet’ or ‘sticky’, and if they stay in contact with sheds for too long, solid deposits are formed that lead to stripper fouling. Extensive fouling decreases stripping efficiency and liquid product yield and can shorten run-times between shutdowns. Because of the fouling, the shape of sheds mostly changes by increasing their surfaces thickness. An early indication of that fouling and the ability to follow its development are essential for choosing optimal parameters of the process. The radioactive particle tracking (RPT) method has been tested to determine its applicability to indicate the change in the shape of internals within a fluidised bed reactor when direct observation is impossible. A single radioactive tracer-particle has been traced in experiments lasting from 2 to 6 h. The experiments were conducted in a lab-scale, cold-flow fluidised bed into which a single shed with walls of different thickness was incorporated. This experimental fluidised bed provides intensive solid phase mixing that allows a single tracer-particle to be located in any place within the reactor. By registering the frequency of the tracer-particle appearance within a defined internal space surrounding the shed, the shape of shed was reconstructed. The conducted experiments suggest that RPT technique allows for tracking internals' fouling within a fluidised bed reactor. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

The stripper section of a fluid-coker consists of a system of baffles (sheds) that enhances the removal efficiency of entrained and adsorbed hydrocarbons from the fluidised coke-particles. If the particles contain a thin liquid film layer of heavy hydrocarbons, making them excessively ‘wet’ or ‘sticky’, and if they stay in contact with sheds for too long, solid deposits are formed that lead to stripper fouling. Extensive fouling decreases stripping efficiency and liquid product yield and can shorten run-times between shutdowns. Because of the fouling, the shape of sheds mostly changes by increasing their surfaces thickness. An early indication of that fouling and the ability to follow its development are essential for choosing optimal parameters of the process. The radioactive particle tracking (RPT) method has been tested to determine its applicability to indicate the change in the shape of internals within a fluidised bed reactor when direct observation is impossible. A single radioactive tracer-particle has been traced in experiments lasting from 2 to 6 h. The experiments were conducted in a lab-scale, cold-flow fluidised bed into which a single shed with walls of different thickness was incorporated. This experimental fluidised bed provides intensive solid phase mixing that allows a single tracer-particle to be located in any place within the reactor. By registering the frequency of the tracer-particle appearance within a defined internal space surrounding the shed, the shape of shed was reconstructed. The conducted experiments suggest that RPT technique allows for tracking internals' fouling within a fluidised bed reactor. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21715" xmlns="http://purl.org/rss/1.0/"><title>Natural gas viscosity estimation using density based models</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21715</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Natural gas viscosity estimation using density based models</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ehsan Heidaryan, Azad Jarrahian</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-07-05T14:38:05.05826-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21715</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21715</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21715</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1183</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1189</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>Accurate value determination of natural gas viscosity plays a key role in its management as it is one of the most important parameters in natural gas engineering calculations. In this study, a comprehensive model is suggested for prediction of natural gas viscosity in a wide range of pressures, temperatures, densities and compositions. The new model can be applicable for gases containing heptane plus and non-hydrocarbon components. It is validated by the 2011 viscosity data from 18 different gas mixtures. Compared to existing similar models and correlations, its results are quite satisfactory. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Accurate value determination of natural gas viscosity plays a key role in its management as it is one of the most important parameters in natural gas engineering calculations. In this study, a comprehensive model is suggested for prediction of natural gas viscosity in a wide range of pressures, temperatures, densities and compositions. The new model can be applicable for gases containing heptane plus and non-hydrocarbon components. It is validated by the 2011 viscosity data from 18 different gas mixtures. Compared to existing similar models and correlations, its results are quite satisfactory. © 2012 Canadian Society for Chemical Engineering
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21727" xmlns="http://purl.org/rss/1.0/"><title>Mass transfer around prolate spheroidal drops in an extensional flow</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21727</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Mass transfer around prolate spheroidal drops in an extensional flow</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Moshe Favelukis, Olga M. Lavrenteva</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-08-08T09:54:20.922092-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cjce.21727</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/cjce.21727</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcjce.21727</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1190</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1199</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>Mass transfer in the continuous phase around a small eccentricity prolate spheroidal drop in an axisymmetric extensional creeping flow and at large Peclet numbers was investigated theoretically. The results show that, at very short times, the total quantity of solute transferred to or from the drop represents, at <em>O</em>(<em>Ca</em><sup>1</sup>), mass transfer by diffusion only around a sphere. For long times, or at steady-state, the total quantity of solute transferred is, at <em>O</em>(<em>Ca</em><sup>1</sup>), slightly smaller than that of a spherical drop, and it decreases with an increase of the capillary number or the viscosity ratio. © 2012 Canadian Society for Chemical Engineering</p></div>
]]></content:encoded><description>

Mass transfer in the continuous phase around a small eccentricity prolate spheroidal drop in an axisymmetric extensional creeping flow and at large Peclet numbers was investigated theoretically. The results show that, at very short times, the total quantity of solute transferred to or from the drop represents, at O(Ca1), mass transfer by diffusion only around a sphere. For long times, or at steady-state, the total quantity of solute transferred is, at O(Ca1), slightly smaller than that of a spherical drop, and it decreases with an increase of the capillary number or the viscosity ratio. © 2012 Canadian Society for Chemical Engineering
</description></item></rdf:RDF>