<?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)1547-5905" xmlns="http://purl.org/rss/1.0/"><title>AIChE Journal</title><description> Wiley Online Library : AIChE Journal</description><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2F%28ISSN%291547-5905</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 American Institute of Chemical Engineers</dc:rights><prism:issn xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">0001-1541</prism:issn><prism:eIssn xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1547-5905</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/">59</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/">1830</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2266</prism:endingPage><image rdf:resource="http://onlinelibrary.wiley.com/store/10.1002/aic.v59.6/asset/cover.gif?v=1&amp;s=77fb84c52f3687340674d868e6125806fcffb58c"/><items><rdf:Seq><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14148"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14145"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14144"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14143"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14141"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14142"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14134"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14140"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14139"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14135"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14137"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14136"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14138"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14128"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14129"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14130"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14117"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14114"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14113"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14105"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14088"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14125"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14133"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14118"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14132"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14122"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14131"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14126"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14124"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14127"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14121"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14120"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14119"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14116"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14110"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14092"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14115"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14099"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14090"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14107"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14093"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14112"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14111"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14098"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14108"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14106"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14104"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14091"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14102"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14101"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14040"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14100"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14097"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14095"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14086"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14096"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14071"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14055"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14061"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14081"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14063"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14084"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14087"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14089"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14083"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14068"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14070"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14024"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14065"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14080"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14076"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14082"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14073"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14079"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14072"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14064"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14074"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14067"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14033"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14060"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14058"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14029"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14052"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14062"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14020"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14044"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14039"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14059"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14057"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14042"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14053"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14046"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14025"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14050"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14054"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14051"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14007"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14012"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14047"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14000"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14027"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14037"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14041"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14036"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14045"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14038"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14035"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14030"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14028"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14017"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14009"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14011"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14026"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14023"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14022"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14018"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14001"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14008"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14019"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14016"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14015"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14014"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14013"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13958"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14006"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14004"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13998"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13965"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.11232"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14123"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13988"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13963"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13968"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13974"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13982"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13999"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13990"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13980"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13997"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13962"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13957"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13964"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13975"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13993"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14010"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13991"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13989"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13969"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13981"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13960"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13979"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13984"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13985"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13987"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13994"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13967"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13966"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13970"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14103"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14109"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13976"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13986"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13973"/></rdf:Seq></items></channel><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14148" xmlns="http://purl.org/rss/1.0/"><title>Energy-water efficiency and U.S. industrial steam</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14148</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Energy-water efficiency and U.S. industrial steam</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Eric Masanet, Michael E. Walker</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-22T01:33:31.793339-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14148</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14148</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14148</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Perspective</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[]]></content:encoded><description/></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14145" xmlns="http://purl.org/rss/1.0/"><title>Simultaneous solution approach to model-based experimental design</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14145</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Simultaneous solution approach to model-based experimental design</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M. D. Hoang, T. Barz, V. A. Merchan, L. T. Biegler, H. Arellano-Garcia</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-17T01:26:23.697117-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14145</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14145</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14145</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>In this work, model-based experimental design is formulated and solved as a large scale NLP problem. The key idea of the proposed approach is the extension of model equations with sensitivity equations forming an extended sensitivities-state equation system. The resulting system is then totally discretized and simultaneously solved as constraints of the NLP problem. Thereby, higher derivatives of the parameter sensitivities with respect to the control variables are directly calculated and exact. This is an advantage in comparison with proposed sequential approaches to model-based experimental design so far, where these derivatives have to be additionally integrated throughout the optimization steps. This can end up in a high computational load especially for systems with many control variables. Furthermore, an advanced sampling strategy is proposed which combines the strength of the optimal sampling design and the variation of the collocation element lengths while fully using the entire optimization space of the simultaneous formulation. © 2013 American Institute of Chemical Engineers AIChE J, 2013</p></div>
]]></content:encoded><description>

In this work, model-based experimental design is formulated and solved as a large scale NLP problem. The key idea of the proposed approach is the extension of model equations with sensitivity equations forming an extended sensitivities-state equation system. The resulting system is then totally discretized and simultaneously solved as constraints of the NLP problem. Thereby, higher derivatives of the parameter sensitivities with respect to the control variables are directly calculated and exact. This is an advantage in comparison with proposed sequential approaches to model-based experimental design so far, where these derivatives have to be additionally integrated throughout the optimization steps. This can end up in a high computational load especially for systems with many control variables. Furthermore, an advanced sampling strategy is proposed which combines the strength of the optimal sampling design and the variation of the collocation element lengths while fully using the entire optimization space of the simultaneous formulation. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14144" xmlns="http://purl.org/rss/1.0/"><title>Reactor modeling and recipe optimization of polyether polyol processes: Polypropylene glycol</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14144</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Reactor modeling and recipe optimization of polyether polyol processes: Polypropylene glycol</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yisu Nie, Lorenz T. Biegler, Carlos M. Villa, John M. Wassick</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-16T23:30:51.096849-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14144</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14144</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14144</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>This paper addresses the reactor modeling and recipe optimization of conventional semi-batch polyether polyol processes, in particular for the polymerization of propylene oxide to make polypropylene glycol. A rigorous mathematical reactor model is first developed to describe the dynamic behavior of the polymerization process based on first-principles including the mass and population balances, reaction kinetics and vapor-liquid equilibria. Next, the obtained differential algebraic model is reformulated by applying a nullspace projection method that results in an equivalent dynamic system with better computational performance. The reactor model is validated against plant data by adjusting model parameters. A dynamic optimization problem is then formulated to optimize the process recipe, where the batch processing time is minimized, given a target product molecular weight as well as other requirements on product quality and process safety. The dynamic optimization problem is translated into a nonlinear program by using the simultaneous collocation strategy and further solved with the interior point method to obtain the optimal control profiles. The case study result shows a good match between the model prediction and real plant data, and the optimization approach is able to significantly reduce the batch time by 47%, which indicates great potential for industrial applications. © 2013 American Institute of Chemical Engineers AIChE J, 2013</p></div>
]]></content:encoded><description>

This paper addresses the reactor modeling and recipe optimization of conventional semi-batch polyether polyol processes, in particular for the polymerization of propylene oxide to make polypropylene glycol. A rigorous mathematical reactor model is first developed to describe the dynamic behavior of the polymerization process based on first-principles including the mass and population balances, reaction kinetics and vapor-liquid equilibria. Next, the obtained differential algebraic model is reformulated by applying a nullspace projection method that results in an equivalent dynamic system with better computational performance. The reactor model is validated against plant data by adjusting model parameters. A dynamic optimization problem is then formulated to optimize the process recipe, where the batch processing time is minimized, given a target product molecular weight as well as other requirements on product quality and process safety. The dynamic optimization problem is translated into a nonlinear program by using the simultaneous collocation strategy and further solved with the interior point method to obtain the optimal control profiles. The case study result shows a good match between the model prediction and real plant data, and the optimization approach is able to significantly reduce the batch time by 47%, which indicates great potential for industrial applications. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14143" xmlns="http://purl.org/rss/1.0/"><title>Energy generation using thermopower waves: Experimental and analytical progress</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14143</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Energy generation using thermopower waves: Experimental and analytical progress</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sayalee G. Mahajan, Qing Hua Wang, Joel T. Abrahamson, Michael S. Strano</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-15T23:36:18.622694-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14143</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14143</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14143</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. Reaction Engineering, 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>Thermopower waves convert chemical energy into electrical power by using nanostructured thermal conduits like carbon nanotubes (CNTs) by taking advantage of their high thermal conductivity to propagate the heat released by an exothermic reaction of a fuel layer coated around the conduit. Electron–phonon coupling in the CNTs then leads to an electrical output. Previous work using cyclotrimethylene-trinitramine coated around multi-walled CNTs has shown electrical output as high as 7 kW kg<sup>-1</sup>.<sup>1</sup> This phenomenon has potential to aid the manufacture of nanoscale power sources capable of releasing large power pulses for specific applications. Researchers have studied the effects of other system properties, including the conduit thermal conductivity, the chemical properties of the fuel, and the coupling of the reactions to inorganic thermoelectric materials. An analytical solution for the governing heat and mass balance equations has also been derived. Here, we review the progress made in the field of thermopower waves. © 2013 American Institute of Chemical Engineers AIChE J, 2013</p></div>
]]></content:encoded><description>

Thermopower waves convert chemical energy into electrical power by using nanostructured thermal conduits like carbon nanotubes (CNTs) by taking advantage of their high thermal conductivity to propagate the heat released by an exothermic reaction of a fuel layer coated around the conduit. Electron–phonon coupling in the CNTs then leads to an electrical output. Previous work using cyclotrimethylene-trinitramine coated around multi-walled CNTs has shown electrical output as high as 7 kW kg-1.1 This phenomenon has potential to aid the manufacture of nanoscale power sources capable of releasing large power pulses for specific applications. Researchers have studied the effects of other system properties, including the conduit thermal conductivity, the chemical properties of the fuel, and the coupling of the reactions to inorganic thermoelectric materials. An analytical solution for the governing heat and mass balance equations has also been derived. Here, we review the progress made in the field of thermopower waves. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14141" xmlns="http://purl.org/rss/1.0/"><title>Generalized generic model control of high-purity internal thermally coupled distillation column based on nonlinear wave theory</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14141</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Generalized generic model control of high-purity internal thermally coupled distillation column based on nonlinear wave theory</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Lin Cong, Xinggao Liu, Yexiang Zhou, Youxian Sun</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-15T23:06:58.400355-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14141</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14141</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14141</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 new model-based control strategy for the internal thermally coupled distillation column (ITCDIC) is presented. Based on the nonlinear wave theory that describes the nonlinear dynamics in the separation processes, a simplified nonlinear wave model is established that concerns both the wave propagation and the profile shape. An advanced controller (WGGMC) is formulated by combining the nonlinear wave model with a generalized generic model control (GGMC). Compared with a conventional generic model controller based on a data-driven model (TGMC) and another wave-model based generic model controller (WGMC) developed in our previous work, WGGMC exhibits the best performances in both servo control and regulatory control. Furthermore, WGGMC can handle a very-high-purity system of ITCDIC with top product composition of 0.99999, while the other two controllers fail to work. © 2013 American Institute of Chemical Engineers AIChE J, 2013</p></div>
]]></content:encoded><description>

A new model-based control strategy for the internal thermally coupled distillation column (ITCDIC) is presented. Based on the nonlinear wave theory that describes the nonlinear dynamics in the separation processes, a simplified nonlinear wave model is established that concerns both the wave propagation and the profile shape. An advanced controller (WGGMC) is formulated by combining the nonlinear wave model with a generalized generic model control (GGMC). Compared with a conventional generic model controller based on a data-driven model (TGMC) and another wave-model based generic model controller (WGMC) developed in our previous work, WGGMC exhibits the best performances in both servo control and regulatory control. Furthermore, WGGMC can handle a very-high-purity system of ITCDIC with top product composition of 0.99999, while the other two controllers fail to work. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14142" xmlns="http://purl.org/rss/1.0/"><title>Enhanced hydroformylation by carbon dioxide-expanded media with soluble Rh complexes in nanofiltration membrane reactors</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14142</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Enhanced hydroformylation by carbon dioxide-expanded media with soluble Rh complexes in nanofiltration membrane reactors</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Zhuanzhuan Xie, Jing Fang, Bala Subramaniam, Swarup K. Maiti, William Snavely, Jon A. Tunge</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-15T22:54:55.821063-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14142</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14142</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14142</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, 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 novel process for continuous hydroformylation in CO<sub>2</sub>-expanded liquids (CXLs) is demonstrated using bulky phosphite ligands that are effectively retained in the stirred reactor by a nanofiltration membrane. The reactor is operated at 50°C with a syngas pressure of 0.6 MPa to avoid CO inhibition of reaction rate and selectivity. The nanofiltration pressure is provided by ~3.2 MPa CO<sub>2</sub> that expands the hydroformylation mixture and increases the H<sub>2</sub>/CO ratio in the CXL phase resulting in enhanced turnover frequency (~340 h<sup>-1</sup>), aldehydes selectivity (&gt;90%) and high regioselectivity (<em>n/i</em> ~8) at nearly steady operation. The use of pressurized CO<sub>2</sub> also reduces the viscosity in the CXL phase thereby improving the mass transfer properties. Constant permeate flux is maintained during the 50 h run with Rh leakage being less than 0.5 ppm. This technology concept has potential applications in homogeneous catalytic processes to improve resource utilization and catalyst containment for practical viability. © 2013 American Institute of Chemical Engineers AIChE J, 2013</p></div>
]]></content:encoded><description>

A novel process for continuous hydroformylation in CO2-expanded liquids (CXLs) is demonstrated using bulky phosphite ligands that are effectively retained in the stirred reactor by a nanofiltration membrane. The reactor is operated at 50°C with a syngas pressure of 0.6 MPa to avoid CO inhibition of reaction rate and selectivity. The nanofiltration pressure is provided by ~3.2 MPa CO2 that expands the hydroformylation mixture and increases the H2/CO ratio in the CXL phase resulting in enhanced turnover frequency (~340 h-1), aldehydes selectivity (&gt;90%) and high regioselectivity (n/i ~8) at nearly steady operation. The use of pressurized CO2 also reduces the viscosity in the CXL phase thereby improving the mass transfer properties. Constant permeate flux is maintained during the 50 h run with Rh leakage being less than 0.5 ppm. This technology concept has potential applications in homogeneous catalytic processes to improve resource utilization and catalyst containment for practical viability. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14134" xmlns="http://purl.org/rss/1.0/"><title>A nanoscale model for characterizing the complex pore structure of biochars</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14134</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A nanoscale model for characterizing the complex pore structure of biochars</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Kyriacos Zygourakis, Hao Sun, Pauline Markenscoff</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-10T03:57:04.909302-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14134</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14134</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14134</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson.Reaction Engineering, 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[]]></content:encoded><description/></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14140" xmlns="http://purl.org/rss/1.0/"><title>Pro-active scheduling of batch processes by a combined robust optimization and multi-parametric programming approach</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14140</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Pro-active scheduling of batch processes by a combined robust optimization and multi-parametric programming approach</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Martina Wittmann-Hohlbein, Efstratios N. Pistikopoulos</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-10T00:25:48.109991-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14140</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14140</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14140</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>We address short-term batch process scheduling problems contaminated with uncertainty in the data. The MILP scheduling model, based on the formulation of Ierapetritou and Floudas<sup>1</sup> (1998), contains parameter dependencies at multiple locations, yielding a general multi-parametric (mp) MILP problem. A pro-active scheduling policy is obtained by solving the partially robust counterpart formulation. The counterpart model may remain a multi-parametric problem, yet it is immunized against uncertainty in the entries of the constraint matrix and against all parameters whose values are not available at the time of decision making. We extend our previous work on the approximate solution of mp-MILP problems, Wittmann-Hohlbein and Pistikopoulos<sup>2</sup> (2012), by embedding different uncertainty sets (box, ellipsoidal and budget parameter regulated uncertainty), and by incorporating information about the availability of uncertain data in the construction of the partially robust scheduling model. For any parameter realization, the corresponding schedule is then obtained through function evaluation. © 2013 American Institute of Chemical Engineers AIChE J, 2013</p></div>
]]></content:encoded><description>

We address short-term batch process scheduling problems contaminated with uncertainty in the data. The MILP scheduling model, based on the formulation of Ierapetritou and Floudas1 (1998), contains parameter dependencies at multiple locations, yielding a general multi-parametric (mp) MILP problem. A pro-active scheduling policy is obtained by solving the partially robust counterpart formulation. The counterpart model may remain a multi-parametric problem, yet it is immunized against uncertainty in the entries of the constraint matrix and against all parameters whose values are not available at the time of decision making. We extend our previous work on the approximate solution of mp-MILP problems, Wittmann-Hohlbein and Pistikopoulos2 (2012), by embedding different uncertainty sets (box, ellipsoidal and budget parameter regulated uncertainty), and by incorporating information about the availability of uncertain data in the construction of the partially robust scheduling model. For any parameter realization, the corresponding schedule is then obtained through function evaluation. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14139" xmlns="http://purl.org/rss/1.0/"><title>Analysis on development of magnetite hollow spheres through one-pot solvothermal process</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14139</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Analysis on development of magnetite hollow spheres through one-pot solvothermal process</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dung T. Nguyen, Kyo-Seon Kim</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-10T00:25:29.655236-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14139</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14139</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14139</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Inorganic Materials: Synthesis and Processing</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="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>Monodisperse magnetite nanospheres with hollow interior structure were synthesized through one-pot solvothermal process, in an isothermal environment at 200<sup>o</sup>C for 12 h, using a sole iron precursor (FeCl<sub>3</sub>.6H<sub>2</sub>O) and without any template. We demonstrated the development of hollow structure of magnetite spheres by characterizing systematically the changes of morphology and crystal structure for different processing times. We also provided the cross-sectional images of the Fe<sub>3</sub>O<sub>4</sub> spheres at different processing times to visualize the hollowing process inside the spheres with time. A detailed process mechanism to form the hollow structure of magnetite spheres was proposed, combining the formation of numerous tiny grains, the spherical assembly of those grains and the chemical conversion of the Fe (III) compounds to generate Fe<sub>3</sub>O<sub>4</sub> simultaneously coupled with the Ostwald ripening process within the magnetite spheres. © 2013 American Institute of Chemical Engineers AIChE J, 2013</p></div>
]]></content:encoded><description>

Monodisperse magnetite nanospheres with hollow interior structure were synthesized through one-pot solvothermal process, in an isothermal environment at 200oC for 12 h, using a sole iron precursor (FeCl3.6H2O) and without any template. We demonstrated the development of hollow structure of magnetite spheres by characterizing systematically the changes of morphology and crystal structure for different processing times. We also provided the cross-sectional images of the Fe3O4 spheres at different processing times to visualize the hollowing process inside the spheres with time. A detailed process mechanism to form the hollow structure of magnetite spheres was proposed, combining the formation of numerous tiny grains, the spherical assembly of those grains and the chemical conversion of the Fe (III) compounds to generate Fe3O4 simultaneously coupled with the Ostwald ripening process within the magnetite spheres. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14135" xmlns="http://purl.org/rss/1.0/"><title>Foaming in wet flue gas desulphurisation plants: Lab-scale investigation of long-term performance of antifoaming agents</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14135</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Foaming in wet flue gas desulphurisation plants: Lab-scale investigation of long-term performance of antifoaming agents</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Siqiang Qin, Brian B. Hansen, Søren Kiil</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-08T23:53:56.424739-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14135</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14135</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14135</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>Spontaneous foaming can cause a range of operational problems in industrial processes such as wet flue gas desulphurisation (FGD). This work investigates the performance of selected antifoaming agents (Nalco FM-37, Foamtrol 2290, and rapeseed oil) on foams generated by egg white albumin (protein), sodium dodecyl sulfate (SDS), and adipic acid at conditions of relevance for wet FGD plants. The addition of antifoaming agents breaks any existing foam and causes an induction period without foaming, after which the foam gradually will begin to reappear. Foaming by egg white albumin (2 g/L) at 0.014 m/s could be controlled by both commercial antifoaming agents (6.4 g/L), but not by rapeseed oil addition. Foaming by pure commercial antifoaming agents has also been demonstrated: up to 7·10<sup>-2</sup> m foam was observed with 6.4 g/L Nalco FM-37. © 2013 American Institute of Chemical Engineers AIChE J, 2013</p></div>
]]></content:encoded><description>

Spontaneous foaming can cause a range of operational problems in industrial processes such as wet flue gas desulphurisation (FGD). This work investigates the performance of selected antifoaming agents (Nalco FM-37, Foamtrol 2290, and rapeseed oil) on foams generated by egg white albumin (protein), sodium dodecyl sulfate (SDS), and adipic acid at conditions of relevance for wet FGD plants. The addition of antifoaming agents breaks any existing foam and causes an induction period without foaming, after which the foam gradually will begin to reappear. Foaming by egg white albumin (2 g/L) at 0.014 m/s could be controlled by both commercial antifoaming agents (6.4 g/L), but not by rapeseed oil addition. Foaming by pure commercial antifoaming agents has also been demonstrated: up to 7·10-2 m foam was observed with 6.4 g/L Nalco FM-37. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14137" xmlns="http://purl.org/rss/1.0/"><title>A new technique for recovering energy in thermally coupled distillation using vapor recompression cycles</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14137</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A new technique for recovering energy in thermally coupled distillation using vapor recompression cycles</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Miguel A. Navarro-Amorós, Rubén Ruiz-Femenia, José A. Caballero</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-08T23:22:00.007926-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14137</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14137</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14137</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>Even though it has been proved that a fully thermally coupled distillation (TCD) system minimizes the energy used by a sequence of columns, it is well known that vapor/liquid transfers between different sections produce an unavoidable excess of vapor (liquid) in some of them, increasing both the investment and operating costs. In this paper we propose to take advantage of this situation by extracting the extra vapor/liquid and subjecting it to a direct/reverse vapor compression cycle. This new arrangement restores the optimal operating conditions of some of the affected sections with energy savings of around 20-30% compared with conventional TCD columns.</p></div>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Various examples, including the direct and reverse vapor recompression cycles, are presented. Furthermore, in each example, all possible modes of distillation (direct, indirect and Petlyuk distillation) with and without vapor recompression cycles (VRC) are compared to ensure that this approach delivers the best results. © 2013 American Institute of Chemical Engineers AIChE J, 2013</p></div>
]]></content:encoded><description>

Even though it has been proved that a fully thermally coupled distillation (TCD) system minimizes the energy used by a sequence of columns, it is well known that vapor/liquid transfers between different sections produce an unavoidable excess of vapor (liquid) in some of them, increasing both the investment and operating costs. In this paper we propose to take advantage of this situation by extracting the extra vapor/liquid and subjecting it to a direct/reverse vapor compression cycle. This new arrangement restores the optimal operating conditions of some of the affected sections with energy savings of around 20-30% compared with conventional TCD columns.
Various examples, including the direct and reverse vapor recompression cycles, are presented. Furthermore, in each example, all possible modes of distillation (direct, indirect and Petlyuk distillation) with and without vapor recompression cycles (VRC) are compared to ensure that this approach delivers the best results. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14136" xmlns="http://purl.org/rss/1.0/"><title>Phase behavior of mixture of supercritical CO2 + ionic liquid: Thermodynamic consistency test of experimental data</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14136</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Phase behavior of mixture of supercritical CO2 + ionic liquid: Thermodynamic consistency test of experimental data</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ali Eslamimanesh, Amir H. Mohammadi, Yousef Salamat, Mohammad-Javad Shojaei, Somayeh Eskandari, Dominique Richon</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-08T23:12:44.980165-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14136</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14136</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14136</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Thermodynamics and Molecular-Scale 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>In this work, we have applied various models composed of the Peng-Robinson Equation of State (PR-EoS) and the Soave-Redlich-Kwong Equation of State (SRK-EoS) associated to three mixing rules including the following: Wong-Sandler (WS), van der Waals one (vdW1), and van der Waals two (vdW2) for phase behavior modeling of mixtures of supercritical CO<sub>2</sub> + different ionic liquids in vapor-liquid equilibrium (VLE) region. We have found that the PR EoS implying the WS mixing rule can be used as a reliable thermodynamic model to perform a thermodynamic consistency test on the experimental data of phase behaviors of the supercritical CO<sub>2</sub> + ionic liquid systems (19 commonly-used ionic liquids have been studied). The results show that 40 % of the experimental data seem to be thermodynamically consistent, 55.5 % seem to be thermodynamically inconsistent, and 4.5 % seem to be not fully consistent. © 2013 American Institute of Chemical Engineers AIChE J, 2013</p></div>
]]></content:encoded><description>

In this work, we have applied various models composed of the Peng-Robinson Equation of State (PR-EoS) and the Soave-Redlich-Kwong Equation of State (SRK-EoS) associated to three mixing rules including the following: Wong-Sandler (WS), van der Waals one (vdW1), and van der Waals two (vdW2) for phase behavior modeling of mixtures of supercritical CO2 + different ionic liquids in vapor-liquid equilibrium (VLE) region. We have found that the PR EoS implying the WS mixing rule can be used as a reliable thermodynamic model to perform a thermodynamic consistency test on the experimental data of phase behaviors of the supercritical CO2 + ionic liquid systems (19 commonly-used ionic liquids have been studied). The results show that 40 % of the experimental data seem to be thermodynamically consistent, 55.5 % seem to be thermodynamically inconsistent, and 4.5 % seem to be not fully consistent. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14138" xmlns="http://purl.org/rss/1.0/"><title>Horizontal reactive distillation for multicomponent chiral resolution</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14138</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Horizontal reactive distillation for multicomponent chiral resolution</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Patrick H. Au-Yeung, Sol M. Resnick, Paul M. Witt, Timothy C. Frank, Felipe A. Donate, Lanny A. Robbins</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-08T23:12:39.776763-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14138</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14138</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14138</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separations: Materials, Devices and 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 novel horizontal reactive distillation apparatus and a new overall process scheme are proposed for continuous multicomponent chiral resolution via reversible enantioselective acylation of a chiral (racemic) substrate by a chiral (racemic) acyl donor. The process enables simultaneous production of up to four enantiomers with enhanced chiral purity. Kinetic studies, miniplant experiments, and process simulation results are described for a model lipase-catalyzed reaction: (R)-enantioselective transesterification of (R,S)-1-n-butoxy-2-propanol with (R,S)-1-methoxy-2-acetoxypropane to produce (R)-1-n-butoxy-2-acetoxypropane, (R)-1-methoxy-2-propanol, and the two unreacted (S)-enantiomers of the (R,S)-reagents. A horizontal, compartmentalized reactive distillation vessel is specified instead of a conventional reactive distillation column to provide longer liquid-phase residence time needed for adequate conversion. Low vapor-traffic pressure drop allows operation under vacuum at reduced temperatures for good enzyme stability and enantioselectivity. The general technology has potential as a means to producing a wide range of chiral synthons used in asymmetric syntheses of chiral pharmaceuticals and other biologically-active products. © 2013 American Institute of Chemical Engineers AIChE J, 2013</p></div>
]]></content:encoded><description>

A novel horizontal reactive distillation apparatus and a new overall process scheme are proposed for continuous multicomponent chiral resolution via reversible enantioselective acylation of a chiral (racemic) substrate by a chiral (racemic) acyl donor. The process enables simultaneous production of up to four enantiomers with enhanced chiral purity. Kinetic studies, miniplant experiments, and process simulation results are described for a model lipase-catalyzed reaction: (R)-enantioselective transesterification of (R,S)-1-n-butoxy-2-propanol with (R,S)-1-methoxy-2-acetoxypropane to produce (R)-1-n-butoxy-2-acetoxypropane, (R)-1-methoxy-2-propanol, and the two unreacted (S)-enantiomers of the (R,S)-reagents. A horizontal, compartmentalized reactive distillation vessel is specified instead of a conventional reactive distillation column to provide longer liquid-phase residence time needed for adequate conversion. Low vapor-traffic pressure drop allows operation under vacuum at reduced temperatures for good enzyme stability and enantioselectivity. The general technology has potential as a means to producing a wide range of chiral synthons used in asymmetric syntheses of chiral pharmaceuticals and other biologically-active products. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14128" xmlns="http://purl.org/rss/1.0/"><title>Prediction of normal melting point of pure substances by a reference series method</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14128</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Prediction of normal melting point of pure substances by a reference series method</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Neima Brauner, Mordechai Shacham</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-28T23:36:40.984742-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14128</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14128</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14128</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 “Reference Series” method of Shacham et. al. (<em>AIChE J</em>. 2013; 59:420–428) is modified to enable prediction of normal melting point temperatures (<em>T<sub>m</sub></em>) of pure substances within experimental error level. A homologous series for which large amount and high precision <em>T<sub>m</sub></em> data are available is used as a “reference” series. To predict <em>T<sub>m</sub></em> for a “target” series Quantitative Property-Property Relationships (QPPRs) are derived to represent the predicted <em>T<sub>m</sub></em> values of the “target” series in terms of the <em>T<sub>m</sub></em> values of the reference series. Two QPPRs are necessary in order to match the odd and even carbon number (<em>n<sub>C</sub></em>) oscillations of <em>T<sub>m</sub></em> in the low <em>n<sub>C</sub></em> region. In the high <em>n<sub>C</sub></em> region the QPPR is adjusted to represent correctly the asymptotic behavior of <em>T<sub>m</sub></em>. It is shown that the method is very useful for consistency analysis of <em>T<sub>m</sub></em> data and enables a reliable prediction of <em>T<sub>m</sub></em> in both the low <em>n<sub>C</sub></em> and high <em>n<sub>C</sub></em> regions. © 2013 American Institute of Chemical Engineers AIChE J, 2013</p></div>
]]></content:encoded><description>

The “Reference Series” method of Shacham et. al. (AIChE J. 2013; 59:420–428) is modified to enable prediction of normal melting point temperatures (Tm) of pure substances within experimental error level. A homologous series for which large amount and high precision Tm data are available is used as a “reference” series. To predict Tm for a “target” series Quantitative Property-Property Relationships (QPPRs) are derived to represent the predicted Tm values of the “target” series in terms of the Tm values of the reference series. Two QPPRs are necessary in order to match the odd and even carbon number (nC) oscillations of Tm in the low nC region. In the high nC region the QPPR is adjusted to represent correctly the asymptotic behavior of Tm. It is shown that the method is very useful for consistency analysis of Tm data and enables a reliable prediction of Tm in both the low nC and high nC regions. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14129" xmlns="http://purl.org/rss/1.0/"><title>Bis (2-mercapto-ethyl) amine modification of macroporous sulfonic resin catalyst in bisphenol-a synthesis</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14129</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Bis (2-mercapto-ethyl) amine modification of macroporous sulfonic resin catalyst in bisphenol-a synthesis</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Baohe Wang, Hao Sun, Jing Zhu, Lili Wang, Shuang Chen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-28T23:35:48.859513-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14129</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14129</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14129</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, 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 novel catalyst for bisphenol-A synthesis was prepared by bis (2-mercapto-ethyl) amine adsorbed on macroporous sulfonic resin through neutralization reaction. The physicochemical properties of two resin catalysts before and after bis (2-mercapto-ethyl) amine absorption were compared by scanning electron microscope and nitrogen adsorption. The kinetic of the new catalyst preparation process was studied and found this is a chemical adsorption and endothermic process. The adsorption rate is mainly controlled by the intra-particle diffusion, affected by boundary layer diffusion and chemical reaction as well. The thermodynamic activation parameters were calculated. Compared with unmodified catalyst, the modified resin catalyst showed higher selectivity and acetone conversion in the continuous bisphenol-A synthesis process. © 2013 American Institute of Chemical Engineers AIChE J, 2013</p></div>
]]></content:encoded><description>

A novel catalyst for bisphenol-A synthesis was prepared by bis (2-mercapto-ethyl) amine adsorbed on macroporous sulfonic resin through neutralization reaction. The physicochemical properties of two resin catalysts before and after bis (2-mercapto-ethyl) amine absorption were compared by scanning electron microscope and nitrogen adsorption. The kinetic of the new catalyst preparation process was studied and found this is a chemical adsorption and endothermic process. The adsorption rate is mainly controlled by the intra-particle diffusion, affected by boundary layer diffusion and chemical reaction as well. The thermodynamic activation parameters were calculated. Compared with unmodified catalyst, the modified resin catalyst showed higher selectivity and acetone conversion in the continuous bisphenol-A synthesis process. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14130" xmlns="http://purl.org/rss/1.0/"><title>Filtered two-fluid models of fluidized gas-particle flows: New constitutive relations</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14130</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Filtered two-fluid models of fluidized gas-particle flows: New constitutive relations</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Christian C. Milioli, Fernando E. Milioli, William Holloway, Kapil Agrawal, Sankaran Sundaresan</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-28T23:35:16.65758-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14130</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14130</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14130</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. Particle Technology and Fluidization</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="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>New constitutive relations for filtered two-fluid models of gas-particle flows are obtained by systematically filtering results generated through highly resolved simulations of a kinetic theory based two-fluid model (TFM). It was found in our earlier studies that the residual correlations appearing in the filtered TFM equations depended principally on the filter size and filtered particle volume fraction. Closer inspection of a large amount of computational data gathered in the present study reveals an additional, systematic dependence of the correction to the drag coefficient on the filtered slip velocity, which serves as a marker for the extent of sub-filter scale inhomogeneity. Furthermore, the residual correlations for the momentum fluxes in the gas and particle phases arising from the sub-filter scale fluctuations are found to be modeled nicely using constitutive relations of the form used in large eddy simulations of single-phase turbulent flows. © 2013 American Institute of Chemical Engineers AIChE J, 2013</p></div>
]]></content:encoded><description>

New constitutive relations for filtered two-fluid models of gas-particle flows are obtained by systematically filtering results generated through highly resolved simulations of a kinetic theory based two-fluid model (TFM). It was found in our earlier studies that the residual correlations appearing in the filtered TFM equations depended principally on the filter size and filtered particle volume fraction. Closer inspection of a large amount of computational data gathered in the present study reveals an additional, systematic dependence of the correction to the drag coefficient on the filtered slip velocity, which serves as a marker for the extent of sub-filter scale inhomogeneity. Furthermore, the residual correlations for the momentum fluxes in the gas and particle phases arising from the sub-filter scale fluctuations are found to be modeled nicely using constitutive relations of the form used in large eddy simulations of single-phase turbulent flows. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14117" xmlns="http://purl.org/rss/1.0/"><title>Stereo-PIV experiments and large eddy simulations of flow fields in stirred tanks with rushton and curved-blade turbines</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14117</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Stereo-PIV experiments and large eddy simulations of flow fields in stirred tanks with rushton and curved-blade turbines</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Zhipeng Li, Ge Song, Yuyun Bao, Zhengming Gao</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-10T03:53:48.9393-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14117</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14117</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14117</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena and Fluid Mechanics</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="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 characteristics in pilot-scale stirred tanks with Rushton and curved-blade turbines were investigated by using stereoscopic particle image velocimetry (SPIV) experiments and large eddy simulation (LES) methods. The velocity and turbulent kinetic energy (TKE) in the impeller discharge regions were carefully resolved with a high resolution SPIV system, and the detailed phase-resolved velocity and TKE profiles were used to validate the LES results. The effects of Reynolds number and blade shape on the flow characteristics were discussed. The LES results of velocity, TKE, and the evolution of trailing vortices were compared with the SPIV experimental data, and good agreement was obtained at various phase angles. The effects of subgrid scale model and hybrid grid with different mesh resolutions on the LES results were investigated. The present study showed that LES is a computationally affordable method for the accurate predictions of the complex flow fields in pilot-scale stirred tanks. © 2013 American Institute of Chemical Engineers AIChE J, 2013</p></div>
]]></content:encoded><description>

The flow characteristics in pilot-scale stirred tanks with Rushton and curved-blade turbines were investigated by using stereoscopic particle image velocimetry (SPIV) experiments and large eddy simulation (LES) methods. The velocity and turbulent kinetic energy (TKE) in the impeller discharge regions were carefully resolved with a high resolution SPIV system, and the detailed phase-resolved velocity and TKE profiles were used to validate the LES results. The effects of Reynolds number and blade shape on the flow characteristics were discussed. The LES results of velocity, TKE, and the evolution of trailing vortices were compared with the SPIV experimental data, and good agreement was obtained at various phase angles. The effects of subgrid scale model and hybrid grid with different mesh resolutions on the LES results were investigated. The present study showed that LES is a computationally affordable method for the accurate predictions of the complex flow fields in pilot-scale stirred tanks. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14114" xmlns="http://purl.org/rss/1.0/"><title>Membrane rejection of non-spherical particles: Modeling and experiment</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14114</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Membrane rejection of non-spherical particles: Modeling and experiment</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Basavaraju Agasanapura, Ruth E. Baltus, Charan Tanneru, Shankararaman Chellam</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-10T03:38:28.117122-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14114</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14114</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14114</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separations: Materials, Devices and 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 rejection coefficient of non-spherical particles from microfiltration membranes has been examined from both theoretical and experimental perspectives. Modeling efforts focused on incorporating the convective hindrance factor for a capsule shaped particle in a cylindrical pore into predictions of the rejection coefficient. First, the convective hindrance factor was approximated using previously reported results for the hydrodynamic resistances experienced by a sphere in a pore. Second, computational fluid dynamics calculations predicted the convective hindrance factor for a capsule in a cylindrical pore. Results from both approaches indicate that including hydrodynamic interactions in predictions of the rejection coefficient has a greater effect for smaller particles and particles with smaller aspect ratio (i.e., close to spherical shape). Rejections of several rod-shaped Gram negative bacteria with aspect ratio from 2 to 5 by clean track-etched membranes were in general agreement with theoretical predictions. © 2013 American Institute of Chemical Engineers AIChE J, 2013</p></div>
]]></content:encoded><description>

The rejection coefficient of non-spherical particles from microfiltration membranes has been examined from both theoretical and experimental perspectives. Modeling efforts focused on incorporating the convective hindrance factor for a capsule shaped particle in a cylindrical pore into predictions of the rejection coefficient. First, the convective hindrance factor was approximated using previously reported results for the hydrodynamic resistances experienced by a sphere in a pore. Second, computational fluid dynamics calculations predicted the convective hindrance factor for a capsule in a cylindrical pore. Results from both approaches indicate that including hydrodynamic interactions in predictions of the rejection coefficient has a greater effect for smaller particles and particles with smaller aspect ratio (i.e., close to spherical shape). Rejections of several rod-shaped Gram negative bacteria with aspect ratio from 2 to 5 by clean track-etched membranes were in general agreement with theoretical predictions. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14113" xmlns="http://purl.org/rss/1.0/"><title>Inventory pinch algorithm for gasoline blend planning</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14113</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Inventory pinch algorithm for gasoline blend planning</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Pedro A. Castillo Castillo, Jeffrey D. Kelly, Vladimir Mahalec</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-10T03:30:18.621357-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14113</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14113</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14113</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>Current gasoline blend scheduling practice is to optimize blend plans via fixed duration (e.g. days) multi-period NLP or MINLP models and schedule blends via interactive simulation. Solutions of multi-period models typically have different blend recipes for each time period. We introduce inventory pinch points and use them to construct an algorithm based on single-period non-linear model to minimize the number of different blend recipes. The algorithm optimizes multi-grade blend recipes for each period delimited by the inventory pinch points and then uses a fine-grid multi-period fixed-recipe MILP to compute blend volumes profile. If MILP is infeasible, corresponding period between the pinch points is subdivided and recipes are re-optimized. In our case studies, solutions are computed in significant less time and are most often within 0.01% of the solutions by multi-period MINLP. Reduced number of blend recipes makes it easier for blend scheduler to create a schedule by interactive simulation. © 2013 American Institute of Chemical Engineers AIChE J, 2013</p></div>
]]></content:encoded><description>

Current gasoline blend scheduling practice is to optimize blend plans via fixed duration (e.g. days) multi-period NLP or MINLP models and schedule blends via interactive simulation. Solutions of multi-period models typically have different blend recipes for each time period. We introduce inventory pinch points and use them to construct an algorithm based on single-period non-linear model to minimize the number of different blend recipes. The algorithm optimizes multi-grade blend recipes for each period delimited by the inventory pinch points and then uses a fine-grid multi-period fixed-recipe MILP to compute blend volumes profile. If MILP is infeasible, corresponding period between the pinch points is subdivided and recipes are re-optimized. In our case studies, solutions are computed in significant less time and are most often within 0.01% of the solutions by multi-period MINLP. Reduced number of blend recipes makes it easier for blend scheduler to create a schedule by interactive simulation. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14105" xmlns="http://purl.org/rss/1.0/"><title>Membrane-based ethylene/ethane separation: The upper bound and beyond</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14105</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Membrane-based ethylene/ethane separation: The upper bound and beyond</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Meha Rungta, Chen Zhang, Liren Xu, William J. Koros</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-27T09:32:40.531023-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14105</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14105</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14105</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. Separations: Materials, Devices and 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>Ethylene/ethane separation via cryogenic distillation is extremely energy-intensive, and membrane separation may provide an attractive alternative. This paper summarizes the ethylene/ethane separation performance using polymeric membranes, and presents an experimental ethylene/ethane polymeric upper bound based on literature data. A theoretical prediction of the ethylene/ethane upper bound is also presented, and shows good agreement with the experimental upper bound. The article further discusses two ways to overcome the polymeric ethylene/ethane upper bound, based on increasing the sorption or diffusion selectivity, and presents a review on advanced membrane types such as facilitated transport membranes, zeolite and metal organic framework based membranes, and carbon molecular sieve membranes. Of these, carbon membranes have shown the potential to surpass the polymeric ethylene/ethane upper bound performance. Further, a convenient, potentially scalable method for tailoring the performance of carbon membranes for ethylene/ethane separation based on tuning the pyrolysis conditions has also been demonstrated. © 2013 American Institute of Chemical Engineers AIChE J, 2013.</p></div>
]]></content:encoded><description>

Ethylene/ethane separation via cryogenic distillation is extremely energy-intensive, and membrane separation may provide an attractive alternative. This paper summarizes the ethylene/ethane separation performance using polymeric membranes, and presents an experimental ethylene/ethane polymeric upper bound based on literature data. A theoretical prediction of the ethylene/ethane upper bound is also presented, and shows good agreement with the experimental upper bound. The article further discusses two ways to overcome the polymeric ethylene/ethane upper bound, based on increasing the sorption or diffusion selectivity, and presents a review on advanced membrane types such as facilitated transport membranes, zeolite and metal organic framework based membranes, and carbon molecular sieve membranes. Of these, carbon membranes have shown the potential to surpass the polymeric ethylene/ethane upper bound performance. Further, a convenient, potentially scalable method for tailoring the performance of carbon membranes for ethylene/ethane separation based on tuning the pyrolysis conditions has also been demonstrated. © 2013 American Institute of Chemical Engineers AIChE J, 2013.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14088" xmlns="http://purl.org/rss/1.0/"><title>Systematic modeling of discrete-continuous optimization models through generalized disjunctive programming</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14088</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Systematic modeling of discrete-continuous optimization models through generalized disjunctive programming</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ignacio E. Grossmann, Francisco Trespalacios</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-08T07:26:04.103324-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14088</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14088</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14088</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. 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>Discrete-continuous optimization problems are commonly modeled in algebraic form as mixed-integer linear or nonlinear programming models. Since these models can be formulated in different ways, leading either to solvable or non-solvable problems, there is a need for a systematic modeling framework that provides a fundamental understanding on the nature of these models. This paper describes a modeling framework, Generalized Disjunctive Programming (GDP), which represents problems in terms of Boolean and continuous variables, allowing the representation of constraints as algebraic equations, disjunctions and logic propositions. This paper provides an overview of major research results that have emerged in this area. Basic concepts are emphasized as well as the major classes of formulations that can be derived. These are illustrated with a number of examples in the area of process systems engineering. As will be shown, GDP provides a structured way for systematically deriving mixed-integer optimization models that exhibit strong continuous relaxations, which often translates into shorter computational times. © 2013 American Institute of Chemical Engineers AIChE J, 2013.</p></div>
]]></content:encoded><description>

Discrete-continuous optimization problems are commonly modeled in algebraic form as mixed-integer linear or nonlinear programming models. Since these models can be formulated in different ways, leading either to solvable or non-solvable problems, there is a need for a systematic modeling framework that provides a fundamental understanding on the nature of these models. This paper describes a modeling framework, Generalized Disjunctive Programming (GDP), which represents problems in terms of Boolean and continuous variables, allowing the representation of constraints as algebraic equations, disjunctions and logic propositions. This paper provides an overview of major research results that have emerged in this area. Basic concepts are emphasized as well as the major classes of formulations that can be derived. These are illustrated with a number of examples in the area of process systems engineering. As will be shown, GDP provides a structured way for systematically deriving mixed-integer optimization models that exhibit strong continuous relaxations, which often translates into shorter computational times. © 2013 American Institute of Chemical Engineers AIChE J, 2013.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14125" xmlns="http://purl.org/rss/1.0/"><title>Purification of flue gas by ionic liquids: Carbon monoxide capture in [bmim][Tf2N]</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14125</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Purification of flue gas by ionic liquids: Carbon monoxide capture in [bmim][Tf2N]</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sona Raeissi, Louw J. Florusse, Cor J. Peters</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-21T15:32:34.872817-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14125</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14125</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14125</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Thermodynamics and Molecular-Scale 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Knowledge of the solubility of carbon monoxide in ionic liquids is important for investigating the potential use of ionic liquids in reactions and gas separations. There is very limited information available on the capacity of ionic liquids to capture CO. The solubility of CO in 1-butyl-3-methylimidazolium bis(trifluoromethylsulfonyl)imide was investigated experimentally up to temperatures and pressures of 460 K and 10 MPa, respectively. The solubility was shown to be only slightly temperature-dependent, and the P–T diagram for a constant composition mixture is concave-downward with a peak in pressure. By comparing the single-gas solubility results of CO with various other gases in the same ionic liquid, it seems that ionic liquids can potentially be used as gas-separating media. However, although the single-gas solubilities vary considerably among some gases, further studies on mixed (multicomponent) gases should be carried out as the presence of other components can influence the solubility of each gas component. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Knowledge of the solubility of carbon monoxide in ionic liquids is important for investigating the potential use of ionic liquids in reactions and gas separations. There is very limited information available on the capacity of ionic liquids to capture CO. The solubility of CO in 1-butyl-3-methylimidazolium bis(trifluoromethylsulfonyl)imide was investigated experimentally up to temperatures and pressures of 460 K and 10 MPa, respectively. The solubility was shown to be only slightly temperature-dependent, and the P–T diagram for a constant composition mixture is concave-downward with a peak in pressure. By comparing the single-gas solubility results of CO with various other gases in the same ionic liquid, it seems that ionic liquids can potentially be used as gas-separating media. However, although the single-gas solubilities vary considerably among some gases, further studies on mixed (multicomponent) gases should be carried out as the presence of other components can influence the solubility of each gas component. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14133" xmlns="http://purl.org/rss/1.0/"><title>Surface force arising from adsorbed graphene oxide in alumina suspensions with different shape and size</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14133</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Surface force arising from adsorbed graphene oxide in alumina suspensions with different shape and size</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hazlina Husin, Yee-Kwong Leong, Jishan Liu, Hyoung Jin Choi, Wen Ling Zhang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-21T15:22:13.668535-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14133</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14133</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14133</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Particle Technology and Fluidization</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The effects of graphene oxide (GO) on the yield stress-pH of α-Al<sub>2</sub>O<sub>3</sub> (alumina) suspensions were investigated. For micron-sized platelet alumina suspensions, micron-sized GO additive increased the maximum yield stress by as much as six-folds. This was attributed to GO-mediated bridging interactions between the platelet particles. This type of bridging interactions was much less effective with submicron-sized, spherical, and irregular shape alumina. Adsorption of the anionic GO reflected by the shift of pH of zero zeta potential to a lower pH is particularly high for platelet alumina. The 1.0 dwb % GO concentration added is sufficient to reinforce each platelet particle–particle bond, assisted by a directed GO–platelet interaction configuration. This is, however, not true with submicron-sized particles as the particle concentration increases sharply with the inverse of the particle diameter to power of 3. Moreover, a GO sheet can adsorb several submicron-sized particles and this does not produce the right interaction configuration. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The effects of graphene oxide (GO) on the yield stress-pH of α-Al2O3 (alumina) suspensions were investigated. For micron-sized platelet alumina suspensions, micron-sized GO additive increased the maximum yield stress by as much as six-folds. This was attributed to GO-mediated bridging interactions between the platelet particles. This type of bridging interactions was much less effective with submicron-sized, spherical, and irregular shape alumina. Adsorption of the anionic GO reflected by the shift of pH of zero zeta potential to a lower pH is particularly high for platelet alumina. The 1.0 dwb % GO concentration added is sufficient to reinforce each platelet particle–particle bond, assisted by a directed GO–platelet interaction configuration. This is, however, not true with submicron-sized particles as the particle concentration increases sharply with the inverse of the particle diameter to power of 3. Moreover, a GO sheet can adsorb several submicron-sized particles and this does not produce the right interaction configuration. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14118" xmlns="http://purl.org/rss/1.0/"><title>Design of semiconductor ternary quantum dots with optimal optoelectronic function</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14118</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Design of semiconductor ternary quantum dots with optimal optoelectronic function</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dimitrios Maroudas, Xu Han, Sumeet C. Pandey</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-21T15:12:04.288627-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14118</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14118</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14118</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. Inorganic Materials: Synthesis and Processing</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The function of nanometer-size quantum dots (QDs) of ternary compound semiconductors, such as In<sub>x</sub>Ga<sub>1−x</sub>As and ZnSe<sub>1−x</sub>Te<sub>x</sub>, used in the fabrication of optoelectronic and photovoltaic devices can be optimized by precise tuning of their electronic band gap through control of the QD composition (x) and diameter. Results on compositional distributions in ternary QDs and how they affect the QDs' electronic band gap are reported. A hierarchical modeling approach is followed that combines first-principles density functional theory calculations and classical Monte Carlo simulations with a continuum model of species transport in spherical nanocrystals. In certain cases, the model predicts the formation of core/shell-like structures with shell regions rich in the surface segregating species. A systematic parametric analysis generates a database of transport properties, which can be used to design post-growth thermal annealing processes that enable the development of thermodynamically stable QDs with optimal electronic properties grown through simple one-step colloidal synthesis techniques. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The function of nanometer-size quantum dots (QDs) of ternary compound semiconductors, such as InxGa1−xAs and ZnSe1−xTex, used in the fabrication of optoelectronic and photovoltaic devices can be optimized by precise tuning of their electronic band gap through control of the QD composition (x) and diameter. Results on compositional distributions in ternary QDs and how they affect the QDs' electronic band gap are reported. A hierarchical modeling approach is followed that combines first-principles density functional theory calculations and classical Monte Carlo simulations with a continuum model of species transport in spherical nanocrystals. In certain cases, the model predicts the formation of core/shell-like structures with shell regions rich in the surface segregating species. A systematic parametric analysis generates a database of transport properties, which can be used to design post-growth thermal annealing processes that enable the development of thermodynamically stable QDs with optimal electronic properties grown through simple one-step colloidal synthesis techniques. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14132" xmlns="http://purl.org/rss/1.0/"><title>Evaluation of wall boundary condition parameters for gas–solids fluidized bed simulations</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14132</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Evaluation of wall boundary condition parameters for gas–solids fluidized bed simulations</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Tingwen Li, Sofiane Benyahia</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-16T15:25:24.046742-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14132</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14132</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14132</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Particle Technology and Fluidization</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Wall boundary conditions for the solids phase have significant effects on numerical predictions of various gas–solids fluidized beds. Several models for the granular flow wall boundary condition are available in the open literature for numerical modeling of gas–solids flow. A model for specularity coefficient used in Johnson and Jackson boundary conditions by Li and Benyahia (Li and Benyahia, AIChE J. 2012;58:2058–2068) is implemented in the open-source CFD code-MFIX. The variable specularity coefficient model provides a physical way to calculate the specularity coefficient needed by the partial-slip boundary conditions for the solids phase. Through a series of two-dimensional numerical simulations of bubbling fluidized bed and circulating fluidized bed riser, the model predicts qualitatively consistent trends to the previous studies. Furthermore, a quantitative comparison is conducted between numerical results of variable and constant specularity coefficients to investigate the effect of spatial and temporal variations in specularity coefficient. Published 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Wall boundary conditions for the solids phase have significant effects on numerical predictions of various gas–solids fluidized beds. Several models for the granular flow wall boundary condition are available in the open literature for numerical modeling of gas–solids flow. A model for specularity coefficient used in Johnson and Jackson boundary conditions by Li and Benyahia (Li and Benyahia, AIChE J. 2012;58:2058–2068) is implemented in the open-source CFD code-MFIX. The variable specularity coefficient model provides a physical way to calculate the specularity coefficient needed by the partial-slip boundary conditions for the solids phase. Through a series of two-dimensional numerical simulations of bubbling fluidized bed and circulating fluidized bed riser, the model predicts qualitatively consistent trends to the previous studies. Furthermore, a quantitative comparison is conducted between numerical results of variable and constant specularity coefficients to investigate the effect of spatial and temporal variations in specularity coefficient. Published 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14122" xmlns="http://purl.org/rss/1.0/"><title>Adiabatic behavior of thermal unstable compounds evaluated by means of dynamic scanning calorimetric (DSC) techniques</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14122</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Adiabatic behavior of thermal unstable compounds evaluated by means of dynamic scanning calorimetric (DSC) techniques</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Roberto Sanchirico</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-16T15:17:15.499466-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14122</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14122</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14122</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The article investigates the possibility of obtaining reliable information on the adiabatic behavior of thermally unstable substances based on the thermokinetic data collected by differential scanning calorimetric experiments. In particular, it is developed a novel numerical algorithm which allows the estimation of the adiabatic onset temperature. Theoretical results are verified considering the thermal decomposition of dicumyl peroxide carried out under different calorimetric conditions. Encouraging results point out that the procedures developed allow the assessment of adiabatic critical parameters that are very close to the values determined during the experiments. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The article investigates the possibility of obtaining reliable information on the adiabatic behavior of thermally unstable substances based on the thermokinetic data collected by differential scanning calorimetric experiments. In particular, it is developed a novel numerical algorithm which allows the estimation of the adiabatic onset temperature. Theoretical results are verified considering the thermal decomposition of dicumyl peroxide carried out under different calorimetric conditions. Encouraging results point out that the procedures developed allow the assessment of adiabatic critical parameters that are very close to the values determined during the experiments. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14131" xmlns="http://purl.org/rss/1.0/"><title>Oxy-fuel combustion for CO2 capture using a CO2-tolerant oxygen transporting membrane</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14131</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Oxy-fuel combustion for CO2 capture using a CO2-tolerant oxygen transporting membrane</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yanying Wei, Yanjie Wang, Jun Tang, Zhong Li, Haihui Wang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-16T14:35:11.668621-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14131</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14131</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14131</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separations: Materials, Devices and 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>CO<sub>2</sub> capture via an oxy-fuel route through the U-shaped (Pr<sub>0.9</sub>La<sub>0.1</sub>)<sub>2</sub>(Ni<sub>0.74</sub>Cu<sub>0.21</sub>Ga<sub>0.05</sub>)O<sub>4+δ</sub> (PLNCG) hollow fiber membrane with 100% CH<sub>4</sub> conversion and 100% CO<sub>2</sub> selectivity for 450 h has been explored for the first time. X-ray diffraction, scanning electron microscopy, and energy dispersive spectroscopy characterizations of the spent hollow fiber membrane have also been investigated. All these results indicate that PLNCG hollow fiber membrane shows excellent reaction performance and good stability under oxy-fuel reaction conditions, which will be a potential rounte for reducing CO<sub>2</sub> emissions worldwide. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
CO2 capture via an oxy-fuel route through the U-shaped (Pr0.9La0.1)2(Ni0.74Cu0.21Ga0.05)O4+δ (PLNCG) hollow fiber membrane with 100% CH4 conversion and 100% CO2 selectivity for 450 h has been explored for the first time. X-ray diffraction, scanning electron microscopy, and energy dispersive spectroscopy characterizations of the spent hollow fiber membrane have also been investigated. All these results indicate that PLNCG hollow fiber membrane shows excellent reaction performance and good stability under oxy-fuel reaction conditions, which will be a potential rounte for reducing CO2 emissions worldwide. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14126" xmlns="http://purl.org/rss/1.0/"><title>Enhanced CO2 adsorption capacity and stability using CaO-based adsorbents treated by hydration</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14126</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Enhanced CO2 adsorption capacity and stability using CaO-based adsorbents treated by hydration</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Shengping Wang, Hui Shen, Shasha Fan, Yujun Zhao, Xinbin Ma, Jinlong Gong</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-16T13:05:43.655079-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14126</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14126</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14126</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Inorganic Materials: Synthesis and Processing</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The synthesis of highly efficient CaO-based sorbents using Ca(Ac)<sub>2</sub> as a precursor and ethanol as a modification agent for CO<sub>2</sub> capture is described. This adsorbent has several characteristics such as large surface area and pore volume and small particle size. The influence of ratio of ethanol and water on CO<sub>2</sub> adsorption capacity was evaluated considering that the ethanol concentration could affect the pore structure of sorbents. The results showed that CaO modified by ethanol solution had a higher carbonization and better stability. Particularly, when the volume ratio of ethanol and water was 3, a performance of adsorption capacity of 74% and conversion of 94% was observed. CaO modified by ethanol solution had a superior performance due to the decrease of grain size and the formation of loose porous structure. The influence of steam on stability of adsorbents at high temperatures was examined, and it was found that with the existence of steam diffusion, the capacity of the sorbent could remain at a higher level and the stability was evidently improved. After 18 cycles of adsorption/desorption process, the capacity remained as high as 65%. It was proposed that dynamic and cyclic steam injection was favorable for preventing the sintering of sorbents and facilitating the diffusion of CO<sub>2</sub>. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The synthesis of highly efficient CaO-based sorbents using Ca(Ac)2 as a precursor and ethanol as a modification agent for CO2 capture is described. This adsorbent has several characteristics such as large surface area and pore volume and small particle size. The influence of ratio of ethanol and water on CO2 adsorption capacity was evaluated considering that the ethanol concentration could affect the pore structure of sorbents. The results showed that CaO modified by ethanol solution had a higher carbonization and better stability. Particularly, when the volume ratio of ethanol and water was 3, a performance of adsorption capacity of 74% and conversion of 94% was observed. CaO modified by ethanol solution had a superior performance due to the decrease of grain size and the formation of loose porous structure. The influence of steam on stability of adsorbents at high temperatures was examined, and it was found that with the existence of steam diffusion, the capacity of the sorbent could remain at a higher level and the stability was evidently improved. After 18 cycles of adsorption/desorption process, the capacity remained as high as 65%. It was proposed that dynamic and cyclic steam injection was favorable for preventing the sintering of sorbents and facilitating the diffusion of CO2. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14124" xmlns="http://purl.org/rss/1.0/"><title>Carbon dioxide-in-water foams stabilized with nanoparticles and surfactant acting in synergy</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14124</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Carbon dioxide-in-water foams stabilized with nanoparticles and surfactant acting in synergy</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Andrew J. Worthen, Steven L. Bryant, Chun Huh, Keith P. Johnston</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-16T10:15:58.027526-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14124</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14124</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14124</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. Soft Matter: Synthesis, Processing and Products</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Synergistic interactions at the interface of nanoparticles (bare colloidal silica) and surfactant (caprylamidopropyl betaine) led to the generation of viscous and stable CO<sub>2</sub>-in-water (C/W) foams with fine texture at 19.4 MPa and 50°C. Interestingly, neither species generated C/W foams alone. The surfactant became cationic in the presence of CO<sub>2</sub> and adsorbed on the hydrophilic silica nanoparticle surfaces resulting in an increase in the carbon dioxide/water/nanoparticle contact angle. The surfactant also adsorbed at the CO<sub>2</sub>–water interface, reducing interfacial tension to allow formation of finer bubbles. The foams were generated in a beadpack and characterized by apparent viscosity measurements both in the beadpack and in a capillary tube viscometer. In addition, the macroscopic foam stability was observed visually. The foam texture and viscosity were tunable by controlling the aqueous phase composition. Foam stability is discussed in terms of lamella drainage, disjoining pressure, interfacial viscosity, and hole formation. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Synergistic interactions at the interface of nanoparticles (bare colloidal silica) and surfactant (caprylamidopropyl betaine) led to the generation of viscous and stable CO2-in-water (C/W) foams with fine texture at 19.4 MPa and 50°C. Interestingly, neither species generated C/W foams alone. The surfactant became cationic in the presence of CO2 and adsorbed on the hydrophilic silica nanoparticle surfaces resulting in an increase in the carbon dioxide/water/nanoparticle contact angle. The surfactant also adsorbed at the CO2–water interface, reducing interfacial tension to allow formation of finer bubbles. The foams were generated in a beadpack and characterized by apparent viscosity measurements both in the beadpack and in a capillary tube viscometer. In addition, the macroscopic foam stability was observed visually. The foam texture and viscosity were tunable by controlling the aqueous phase composition. Foam stability is discussed in terms of lamella drainage, disjoining pressure, interfacial viscosity, and hole formation. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14127" xmlns="http://purl.org/rss/1.0/"><title>Anaerobic CO2 fixation by the acetogenic bacterium Moorella thermoacetica</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14127</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Anaerobic CO2 fixation by the acetogenic bacterium Moorella thermoacetica</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Peng Hu, Hamid Rismani-Yazdi, Gregory Stephanopoulos</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-16T09:47:29.674093-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14127</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14127</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14127</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. Biomolecular Engineering, Bioengineering, Biochemicals, Biofuels, and Food</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Anaerobic bacteria such as Moorella thermoacetica have the capacity of fixing carbon dioxide with carbon monoxide and hydrogen for the production of ethanol, acetic acid, and other useful chemicals. In this study, we evaluated the fixation of CO<sub>2</sub> for the production of acetic acid, as a product in its own right but also as precursor for lipid synthesis by oleaginous organisms. We achieved maximum cell optical density of 11.3, acetic acid titer of 31 g/L, and productivity of 0.55 g/L-h at CO mass-transfer rate of 83 mM/h. We also showed electron availability by CO mass transfer limited the process at CO mass transfer rates lower than 30 mM/h. Further enhancement of mass-transfer rate removed such limitations in favor of biological kinetics as main limitation. This work underlines the potential of microbial processes for converting syngas to fuel and chemical products in processes suitable for distributed feedstock utilization. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Anaerobic bacteria such as Moorella thermoacetica have the capacity of fixing carbon dioxide with carbon monoxide and hydrogen for the production of ethanol, acetic acid, and other useful chemicals. In this study, we evaluated the fixation of CO2 for the production of acetic acid, as a product in its own right but also as precursor for lipid synthesis by oleaginous organisms. We achieved maximum cell optical density of 11.3, acetic acid titer of 31 g/L, and productivity of 0.55 g/L-h at CO mass-transfer rate of 83 mM/h. We also showed electron availability by CO mass transfer limited the process at CO mass transfer rates lower than 30 mM/h. Further enhancement of mass-transfer rate removed such limitations in favor of biological kinetics as main limitation. This work underlines the potential of microbial processes for converting syngas to fuel and chemical products in processes suitable for distributed feedstock utilization. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14121" xmlns="http://purl.org/rss/1.0/"><title>Experimental investigation of hysteretic dynamic effect in capillary pressure–saturation relationship for two-phase flow in porous media</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14121</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Experimental investigation of hysteretic dynamic effect in capillary pressure–saturation relationship for two-phase flow in porous media</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mahsanam Mirzaei, Diganta Bhusan Das</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-13T09:01:54.826452-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14121</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14121</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14121</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena and Fluid Mechanics</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p><em>Well-defined laboratory experiments have been carried out to investigate hysteretic dynamic effect in capillary pressure–saturation relationships for two-phase flow in homogeneous and heterogeneous (layered) porous media. Conceptually, the dependence of the capillary pressure curves on the rate of change of saturation (</em>dS<em><sub>w</sub>/</em>dt<em>) is defined as the dynamic effect in capillary pressure relationship, which is indicated by a dynamic coefficient,</em> τ <em>(Pa s) and it determines the rate at which two-phase flow equilibrium is reached, i.e.,</em> dS<em><sub>w</sub>/</em>dt <em>= 0 where</em> S<em><sub>w</sub> and</em> t <em>are the water saturation and time, respectively. The dependences of</em> τ <em>on various fluid and porous materials properties have been studied in the context of drainage; but, there is limited study for imbibition and the hysteresis of</em> τ<em>−</em>S<em><sub>w</sub> relationships. As such, the emphasis in this article is on reporting</em> τ<em>−</em>S<em><sub>w</sub> curves for imbibition while also demonstrating the hysteresis in the</em> τ<em>−</em>S<em><sub>w</sub> relationships by comparing</em> τ<em>−</em>S<em><sub>w</sub> curves for drainage (previously reported) and imbibition (this study) in carefully designed laboratory experiments. Homogeneous sand samples composed of either fine (small particle size and lower permeability) or coarse (larger particle size and higher permeability) sand have been used for these experiments. Furthermore, a layered domain made of a find sand layer sandwiched between two coarse sand layers is used as a model of heterogeneous domain. The results of the study confirm that the</em> τ<em>−</em>S<em><sub>w</sub> relationships are hysteretic in nature and, as such, the speed to flow equilibrium should vary depending on whether drainage or imbibition takes place. At a particular water saturation, the magnitudes of the dynamic coefficient (τ) are found to be generally higher for imbibition, which imply that the speed to flow equilibrium at the same saturation will be slower for imbibition</em>. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Well-defined laboratory experiments have been carried out to investigate hysteretic dynamic effect in capillary pressure–saturation relationships for two-phase flow in homogeneous and heterogeneous (layered) porous media. Conceptually, the dependence of the capillary pressure curves on the rate of change of saturation (dSw/dt) is defined as the dynamic effect in capillary pressure relationship, which is indicated by a dynamic coefficient, τ (Pa s) and it determines the rate at which two-phase flow equilibrium is reached, i.e., dSw/dt = 0 where Sw and t are the water saturation and time, respectively. The dependences of τ on various fluid and porous materials properties have been studied in the context of drainage; but, there is limited study for imbibition and the hysteresis of τ−Sw relationships. As such, the emphasis in this article is on reporting τ−Sw curves for imbibition while also demonstrating the hysteresis in the τ−Sw relationships by comparing τ−Sw curves for drainage (previously reported) and imbibition (this study) in carefully designed laboratory experiments. Homogeneous sand samples composed of either fine (small particle size and lower permeability) or coarse (larger particle size and higher permeability) sand have been used for these experiments. Furthermore, a layered domain made of a find sand layer sandwiched between two coarse sand layers is used as a model of heterogeneous domain. The results of the study confirm that the τ−Sw relationships are hysteretic in nature and, as such, the speed to flow equilibrium should vary depending on whether drainage or imbibition takes place. At a particular water saturation, the magnitudes of the dynamic coefficient (τ) are found to be generally higher for imbibition, which imply that the speed to flow equilibrium at the same saturation will be slower for imbibition. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14120" xmlns="http://purl.org/rss/1.0/"><title>Effect of ring-type internals on solids distribution in a dual circulating fluidized bed system—cold flow model study</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14120</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of ring-type internals on solids distribution in a dual circulating fluidized bed system—cold flow model study</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Diana Carolina Guío-Pérez, Hermann Hofbauer, Tobias Pröll</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-07T09:33:40.071834-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14120</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14120</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14120</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Particle Technology and Fluidization</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The redistribution of solids in a counter-current circulating fluidized bed (CFB) by effect of ring-type internals was investigated in a downscaled cold-flow model. The system consists of two interconnected CFB reactors, in which the primary reactor operates like a common riser while the secondary reactor operates in counter-current. The unit works without circulation rate control devices and the inventory splits inherently between the two reactors by pressure balance and depending on the fluidization velocities. Previous studies showed an increment in the total pressure drop in the secondary reactor as result of the internals installation. With the purpose of obtaining comparable inventory in the secondary reactor with and without rings, a device for adjustment of total inventory was designed and installed. Effects of the aperture ratio, number of rings, fluidization velocity, and particles circulation rate were studied. The results obtained approach a guideline for the detailed design of similar configurations. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The redistribution of solids in a counter-current circulating fluidized bed (CFB) by effect of ring-type internals was investigated in a downscaled cold-flow model. The system consists of two interconnected CFB reactors, in which the primary reactor operates like a common riser while the secondary reactor operates in counter-current. The unit works without circulation rate control devices and the inventory splits inherently between the two reactors by pressure balance and depending on the fluidization velocities. Previous studies showed an increment in the total pressure drop in the secondary reactor as result of the internals installation. With the purpose of obtaining comparable inventory in the secondary reactor with and without rings, a device for adjustment of total inventory was designed and installed. Effects of the aperture ratio, number of rings, fluidization velocity, and particles circulation rate were studied. The results obtained approach a guideline for the detailed design of similar configurations. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14119" xmlns="http://purl.org/rss/1.0/"><title>Bayesian inference and joint probability analysis for batch process monitoring</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14119</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Bayesian inference and joint probability analysis for batch process monitoring</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Zhiqiang Ge, Zhihuan Song</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-03T10:36:29.483762-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14119</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14119</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14119</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A new probabilistic monitoring method for batch processes that have multiple operating conditions is described. Particularly, for multiphase batch processes, a phase-based Bayesian inference strategy is introduced, which can efficiently combine the information of multiple operation modes together into a single model in each specific phase. Therefore, without any process knowledge, local monitoring results in different operation modes can be automatically integrated. Besides, the information of the operation mode can be obtained through joint probability analysis under the Bayesian monitoring framework. Potential extensions of the proposed method for fault diagnosis and identification are also discussed. A benchmark case study on the penicillin fermentation process is given to evaluate the feasibility and efficiency of the proposed method. It is demonstrated that the monitoring performance and the process comprehension have both been improved. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
A new probabilistic monitoring method for batch processes that have multiple operating conditions is described. Particularly, for multiphase batch processes, a phase-based Bayesian inference strategy is introduced, which can efficiently combine the information of multiple operation modes together into a single model in each specific phase. Therefore, without any process knowledge, local monitoring results in different operation modes can be automatically integrated. Besides, the information of the operation mode can be obtained through joint probability analysis under the Bayesian monitoring framework. Potential extensions of the proposed method for fault diagnosis and identification are also discussed. A benchmark case study on the penicillin fermentation process is given to evaluate the feasibility and efficiency of the proposed method. It is demonstrated that the monitoring performance and the process comprehension have both been improved. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14116" xmlns="http://purl.org/rss/1.0/"><title>A graphical approach to process synthesis and its application to steam reforming</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14116</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A graphical approach to process synthesis and its application to steam reforming</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">James Alistair Fox, Diane Hildebrandt, David Glasser, Bilal Patel</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-03T02:16:42.498892-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14116</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14116</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14116</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>It is common practice in chemical engineering to design processes sequentially. The type of product desired determines the choice of the feed materials that are introduced into the reactor networks. These in turn lead into the separation networks. The flows of heat and work are the final part of the sequence to be considered, with the application of heat exchanger networks, and any deficiency or excess in these flows is usually compensated for with the use of utilities. Although the ongoing research into reactor, separation, and heat exchanger optimization is of indubitable value, an aspect that is often overlooked in conventional research is the question: How do changes to one of the elements in the sequence affect the others? Most process designers do not address such matters until the next optimization of the sequence begins. The result of this sequential approach to design is that processes may contain a few very efficient units, but may also have others that are highly inefficient. A graphical technique that incorporates the flows of heat and work into the design of the process at a very early stage is proposed. The technique can be used to prepare flow sheets that represent a synthesized version of the elements that make up the complete process, rendering each component highly efficient. This new design tool uses the thermodynamic properties of enthalpy (representative of process heat requirements) and Gibbs free energy (representative of process work requirements) to develop process flow sheets that operate as close to reversibly as possible, and can be used as a foundation for more detailed refinements to achieve the best possible result. A case was described in a previous paper in which the graphical technique was applied to gasification. The application of the technique to the production of syngas by the steam reforming of natural gas is detailed. We show that the steam reforming process can be operated with increased reversibility and can actually consume carbon dioxide, thus representing a process with a carbon efficiency of greater than 100%, if the way in which all the process units interact with one another is used to utmost advantage. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
It is common practice in chemical engineering to design processes sequentially. The type of product desired determines the choice of the feed materials that are introduced into the reactor networks. These in turn lead into the separation networks. The flows of heat and work are the final part of the sequence to be considered, with the application of heat exchanger networks, and any deficiency or excess in these flows is usually compensated for with the use of utilities. Although the ongoing research into reactor, separation, and heat exchanger optimization is of indubitable value, an aspect that is often overlooked in conventional research is the question: How do changes to one of the elements in the sequence affect the others? Most process designers do not address such matters until the next optimization of the sequence begins. The result of this sequential approach to design is that processes may contain a few very efficient units, but may also have others that are highly inefficient. A graphical technique that incorporates the flows of heat and work into the design of the process at a very early stage is proposed. The technique can be used to prepare flow sheets that represent a synthesized version of the elements that make up the complete process, rendering each component highly efficient. This new design tool uses the thermodynamic properties of enthalpy (representative of process heat requirements) and Gibbs free energy (representative of process work requirements) to develop process flow sheets that operate as close to reversibly as possible, and can be used as a foundation for more detailed refinements to achieve the best possible result. A case was described in a previous paper in which the graphical technique was applied to gasification. The application of the technique to the production of syngas by the steam reforming of natural gas is detailed. We show that the steam reforming process can be operated with increased reversibility and can actually consume carbon dioxide, thus representing a process with a carbon efficiency of greater than 100%, if the way in which all the process units interact with one another is used to utmost advantage. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14110" xmlns="http://purl.org/rss/1.0/"><title>Stability and instability in isothermal CFSTRs with complex chemistry: Some recent results</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14110</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Stability and instability in isothermal CFSTRs with complex chemistry: Some recent results</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Guy Shinar, Daniel Knight, Haixia Ji, Martin Feinberg</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-01T12:56:37.265425-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14110</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14110</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14110</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. Reaction Engineering, 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Although the classical 1955 paper by Bilous and Amundson was largely devoted to the study of nonisothermal systems, they also found it worthwhile to establish the stable behavior of a model isothermal multireaction continuous flow stirred tank reactor for all values of residence time, rate constants, and feed concentrations. Over a half century later, there remains a predisposition to the idea that isothermal reactors are prone to dull, stable behavior even when the underlying chemistry is complex. That idea is revisited in light of some recent findings in chemical reaction network theory. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Although the classical 1955 paper by Bilous and Amundson was largely devoted to the study of nonisothermal systems, they also found it worthwhile to establish the stable behavior of a model isothermal multireaction continuous flow stirred tank reactor for all values of residence time, rate constants, and feed concentrations. Over a half century later, there remains a predisposition to the idea that isothermal reactors are prone to dull, stable behavior even when the underlying chemistry is complex. That idea is revisited in light of some recent findings in chemical reaction network theory. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14092" xmlns="http://purl.org/rss/1.0/"><title>Reactive coupling between immiscible polymer chains: Acceleration by compressive flow</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14092</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Reactive coupling between immiscible polymer chains: Acceleration by compressive flow</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jie Song, Adam M. Baker, Christopher W. Macosko, Randy H. Ewoldt</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-01T09:51:36.01127-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14092</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14092</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14092</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. Reaction Engineering, 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>It is demonstrated that processing flow affects the kinetics of the interfacial coupling reaction between functional groups that are grafted to polymer chains. At melt temperatures the amine group on the end of nylon 6 chains reacts with maleic anhydride grafted polyethylene (PE-MA) and forms graft copolymers. Bilayers were made by lamination and coextrusion and adhesion was measured using asymmetric dual cantilever beam (ADCB). The amount of graft copolymer in the interface was quantified by X-ray photon spectroscopy (XPS). With quiescent lamination, adhesion increased with temperature and the concentration of PE-MA. The adhesion metric, G<sub>c</sub> (critical energy release rate), plotted as a function of Σ (interfacial copolymer density) fell on the same master curve, unifying reaction process, temperature and time. G<sub>c</sub> was a linear function of Σ for low-copolymer coverage and weak adhesion. For relatively high coverage and strong adhesion, G<sub>c</sub> scaled with Σ.<a href="#aic14092-bib-0002" rel="references:#aic14092-bib-0002"/> Coextrusion with compressive flow resulted in a reaction rate strikingly two-orders of magnitude faster than that without compressive flow. The rate in the noncompressive die was close to quiescent lamination. Even for lamination, when compressive flow was applied normal to the interface, the coupling reaction rate was also greatly accelerated. Several mechanisms are speculated for this remarkable acceleration in polymer chain coupling. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
It is demonstrated that processing flow affects the kinetics of the interfacial coupling reaction between functional groups that are grafted to polymer chains. At melt temperatures the amine group on the end of nylon 6 chains reacts with maleic anhydride grafted polyethylene (PE-MA) and forms graft copolymers. Bilayers were made by lamination and coextrusion and adhesion was measured using asymmetric dual cantilever beam (ADCB). The amount of graft copolymer in the interface was quantified by X-ray photon spectroscopy (XPS). With quiescent lamination, adhesion increased with temperature and the concentration of PE-MA. The adhesion metric, Gc (critical energy release rate), plotted as a function of Σ (interfacial copolymer density) fell on the same master curve, unifying reaction process, temperature and time. Gc was a linear function of Σ for low-copolymer coverage and weak adhesion. For relatively high coverage and strong adhesion, Gc scaled with Σ. Coextrusion with compressive flow resulted in a reaction rate strikingly two-orders of magnitude faster than that without compressive flow. The rate in the noncompressive die was close to quiescent lamination. Even for lamination, when compressive flow was applied normal to the interface, the coupling reaction rate was also greatly accelerated. Several mechanisms are speculated for this remarkable acceleration in polymer chain coupling. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14115" xmlns="http://purl.org/rss/1.0/"><title>Pseudo two-dimensional modeling of sediment build-up in centrifuges: A compartment approach using compressional rheology</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14115</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Pseudo two-dimensional modeling of sediment build-up in centrifuges: A compartment approach using compressional rheology</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Lars E. Spelter, Hermann Nirschl, Anthony D. Stickland, Peter J. Scales</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-01T09:22:44.201794-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14115</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14115</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14115</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separations: Materials, Devices and 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Both a new modeling approach and new experimental data for the sediment build-up in centrifuges are presented. In semibatch apparatus, the suspension is continuously fed to the centrifuge, separating the particles inside the rotor and discharging the clarified liquid. The solid phase is removed once the capacity of the centrifuge is reached. The solids fraction of the sediment depends on the rheological properties of the cake. The sediment growth and consolidation throughout the process can be calculated using a pseudo two-dimensional approach that takes into account particle-size dependent settling, sediment compressibility, the centrifugal force field, and the geometry of the bowl. The predictions of the separation behavior and the particle-size distributions of the sediment and overflow are compared with experimentally obtained results, showing improved accuracy when compared to simpler models. The model presented is applicable to all solid-bowl centrifuges without conveying systems. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Both a new modeling approach and new experimental data for the sediment build-up in centrifuges are presented. In semibatch apparatus, the suspension is continuously fed to the centrifuge, separating the particles inside the rotor and discharging the clarified liquid. The solid phase is removed once the capacity of the centrifuge is reached. The solids fraction of the sediment depends on the rheological properties of the cake. The sediment growth and consolidation throughout the process can be calculated using a pseudo two-dimensional approach that takes into account particle-size dependent settling, sediment compressibility, the centrifugal force field, and the geometry of the bowl. The predictions of the separation behavior and the particle-size distributions of the sediment and overflow are compared with experimentally obtained results, showing improved accuracy when compared to simpler models. The model presented is applicable to all solid-bowl centrifuges without conveying systems. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14099" xmlns="http://purl.org/rss/1.0/"><title>Solution-processable exfoliated zeolite nanosheets purified by density gradient centrifugation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14099</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Solution-processable exfoliated zeolite nanosheets purified by density gradient centrifugation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Kumar Varoon Agrawal, Berna Topuz, Zheyu Jiang, Kevin Nguenkam, Bahman Elyassi, Lorraine F. Francis, Michael Tsapatsis, Marta Navarro</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-01T08:56:37.302026-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14099</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14099</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14099</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. Separations: Materials, Devices and 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Highly crystalline exfoliated MFI-nanosheets can pave the way for large-scale deployment of sub-500-nm zeolite membranes due to their processing and packing advantages. Exfoliated MFI-nanosheets prepared by melt compounding contain a large amount of polymer and unexfoliated particles which are detrimental to the fabrication of ultrathin zeolite membranes. Complete removal of polystyrene from the nanosheet suspension in toluene is demonstrated by centrifugation of the suspension across chlorobenzene as confirmed by thermogravimetric analysis (TGA) data and transmission electron microscopy (TEM) images. Rate-zonal centrifugation in a nonlinear density gradient fractionated exfoliated MFI-nanosheets from unexfoliated particles. The purified nanosheets were highly crystalline as indicated by high-resolution TEM (HRTEM) and electron diffraction (ED). Coating of purified MFI-nanosheets on a smooth <em>α-</em>alumina support, fabricated by filtration of <em>α-</em>alumina suspension, led to a compact, b-oriented, 80-nm-thick film. A mild hydrothermal treatment of the film led to a 200-nm-thick membrane, which demonstrated molecular sieving properties. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Highly crystalline exfoliated MFI-nanosheets can pave the way for large-scale deployment of sub-500-nm zeolite membranes due to their processing and packing advantages. Exfoliated MFI-nanosheets prepared by melt compounding contain a large amount of polymer and unexfoliated particles which are detrimental to the fabrication of ultrathin zeolite membranes. Complete removal of polystyrene from the nanosheet suspension in toluene is demonstrated by centrifugation of the suspension across chlorobenzene as confirmed by thermogravimetric analysis (TGA) data and transmission electron microscopy (TEM) images. Rate-zonal centrifugation in a nonlinear density gradient fractionated exfoliated MFI-nanosheets from unexfoliated particles. The purified nanosheets were highly crystalline as indicated by high-resolution TEM (HRTEM) and electron diffraction (ED). Coating of purified MFI-nanosheets on a smooth α-alumina support, fabricated by filtration of α-alumina suspension, led to a compact, b-oriented, 80-nm-thick film. A mild hydrothermal treatment of the film led to a 200-nm-thick membrane, which demonstrated molecular sieving properties. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14090" xmlns="http://purl.org/rss/1.0/"><title>Reactive adsorption for the selective dehydration of sugars to furans: Modeling and experiments</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14090</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Reactive adsorption for the selective dehydration of sugars to furans: Modeling and experiments</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">T. Dallas Swift, Christina Bagia, Vladimiros Nikolakis, Dionisios G. Vlachos, George Peklaris, Paul Dornath, Wei Fan</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-30T15:27:56.499392-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14090</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14090</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14090</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. Reaction Engineering, 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>5-hydroxymethylfurfural (HMF) can be produced from the acid-catalyzed dehydration of fructose, but its yield is limited due to subsequent HMF degradation to side products. A reactive adsorption process is proposed to improve the yield to HMF. Separate experimental single-component isotherms of fructose, HMF, formic acid, and levulinic acid on carbon BP2000 and reaction kinetics of the fructose dehydration to HMF in aqueous solution of HCl are presented to develop empirical isotherms and kinetic rate constants, respectively. These submodels are subsequently integrated in an adsorptive reactor at a range of temperatures (100–150<sup>°</sup>C) with different loadings of adsorbent. It is shown that the adsorbent improves HMF yield compared to the single-solution phase (adsorbent-free case). Low temperatures and high-adsorbent loadings improve HMF yield. Under certain conditions both reactive adsorption and the commonly used reactive extraction can result in a similar improvement in HMF yield. HMF recovery from the solid adsorbent has been identified as a major challenge that can be ameliorated through adsorbent and solvent selection. The framework outlined here can be applied to any aqueous phase chemistry where the desired product is an intermediate in a reaction cascade. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
5-hydroxymethylfurfural (HMF) can be produced from the acid-catalyzed dehydration of fructose, but its yield is limited due to subsequent HMF degradation to side products. A reactive adsorption process is proposed to improve the yield to HMF. Separate experimental single-component isotherms of fructose, HMF, formic acid, and levulinic acid on carbon BP2000 and reaction kinetics of the fructose dehydration to HMF in aqueous solution of HCl are presented to develop empirical isotherms and kinetic rate constants, respectively. These submodels are subsequently integrated in an adsorptive reactor at a range of temperatures (100–150°C) with different loadings of adsorbent. It is shown that the adsorbent improves HMF yield compared to the single-solution phase (adsorbent-free case). Low temperatures and high-adsorbent loadings improve HMF yield. Under certain conditions both reactive adsorption and the commonly used reactive extraction can result in a similar improvement in HMF yield. HMF recovery from the solid adsorbent has been identified as a major challenge that can be ameliorated through adsorbent and solvent selection. The framework outlined here can be applied to any aqueous phase chemistry where the desired product is an intermediate in a reaction cascade. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14107" xmlns="http://purl.org/rss/1.0/"><title>Model-based design of a plant-wide control strategy for a continuous pharmaceutical plant</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14107</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Model-based design of a plant-wide control strategy for a continuous pharmaceutical plant</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Richard Lakerveld, Brahim Benyahia, Richard D. Braatz, Paul I. Barton</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-25T11:55:13.80815-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14107</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14107</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14107</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The design of an effective plant-wide control strategy is a key challenge for the development of future continuous pharmaceutical processes. This article presents a case study for the design of a plant-wide control structure for a system inspired by an end-to-end continuous pharmaceutical pilot plant. A hierarchical decomposition strategy is used to classify control objectives. A plant-wide dynamic model of the process is used to generate parametric sensitivities, which provide a basis for the synthesis of control loops. Simulations for selected disturbances illustrate that the critical quality attributes (CQAs) of the final product can be kept close to specification in the presence of significant and persistent disturbances. Furthermore, it is illustrated how selected CQAs of the final product can be brought simultaneously to a new setpoint while maintaining the remaining CQAs at a constant value during this transition. The latter result shows flexibility to control CQAs independently of each other. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The design of an effective plant-wide control strategy is a key challenge for the development of future continuous pharmaceutical processes. This article presents a case study for the design of a plant-wide control structure for a system inspired by an end-to-end continuous pharmaceutical pilot plant. A hierarchical decomposition strategy is used to classify control objectives. A plant-wide dynamic model of the process is used to generate parametric sensitivities, which provide a basis for the synthesis of control loops. Simulations for selected disturbances illustrate that the critical quality attributes (CQAs) of the final product can be kept close to specification in the presence of significant and persistent disturbances. Furthermore, it is illustrated how selected CQAs of the final product can be brought simultaneously to a new setpoint while maintaining the remaining CQAs at a constant value during this transition. The latter result shows flexibility to control CQAs independently of each other. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14093" xmlns="http://purl.org/rss/1.0/"><title>Covalent crosslinked assembly of tubular ceramic-based multilayer nanofiltration membranes for dye desalination</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14093</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Covalent crosslinked assembly of tubular ceramic-based multilayer nanofiltration membranes for dye desalination</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Lu Wang, Naixin Wang, Guojun Zhang, Shulan Ji</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-25T10:14:27.225852-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14093</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14093</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14093</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separations: Materials, Devices and 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A tubular ceramic-based multilayer composite nanofiltration membrane has been developed for dye desalination. Poly(acrylic acid)(PAA)/poly(vinyl alcohol)(PVA)/glutaraldehyde(GA) was dynamically assembled on to the inner surfaces of tubular ceramic microporous substrates which had been pretreated using dynasylan ameo silane coupling agents. Subsequently, the composite membranes were thermally crosslinked to form covalent ester bonds. Experimental results proved that the composite membrane had good nanofiltration performance for dye desalination. The (GA/PVA/PAA)<sub>3</sub>/ceramic multilayer membrane shows over 96% retention of Congo red and less than 3% NaCl retention using a permeate flux of about 25 L/(m<sup>2</sup>·h). An investigation of membrane performance as a function of operating conditions suggested that the covalent crosslinking multilayer membrane possessed much higher stability compared to other, electrostatically assembled, multilayer membranes. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
A tubular ceramic-based multilayer composite nanofiltration membrane has been developed for dye desalination. Poly(acrylic acid)(PAA)/poly(vinyl alcohol)(PVA)/glutaraldehyde(GA) was dynamically assembled on to the inner surfaces of tubular ceramic microporous substrates which had been pretreated using dynasylan ameo silane coupling agents. Subsequently, the composite membranes were thermally crosslinked to form covalent ester bonds. Experimental results proved that the composite membrane had good nanofiltration performance for dye desalination. The (GA/PVA/PAA)3/ceramic multilayer membrane shows over 96% retention of Congo red and less than 3% NaCl retention using a permeate flux of about 25 L/(m2·h). An investigation of membrane performance as a function of operating conditions suggested that the covalent crosslinking multilayer membrane possessed much higher stability compared to other, electrostatically assembled, multilayer membranes. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14112" xmlns="http://purl.org/rss/1.0/"><title>Optimization-based framework for computer-aided molecular design</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14112</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Optimization-based framework for computer-aided molecular design</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Apurva P. Samudra, Nikolaos V. Sahinidis</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-25T09:58:36.63074-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14112</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14112</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14112</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A new framework to automate, augment, and accelerate steps in computer-aided molecular design is presented. The problem is tackled in three stages: (1) composition design, (2) structure determination, and (3) extended design. Composition identification and structure determination are decoupled to achieve computational efficiency. Using approximate group-contribution methods in the first stage, molecular compositions that fit design targets are identified. In the second stage, isomer structures of solution compositions are determined systematically, and structure-based property corrections are used to refine the solution pool. In the final stage, the design is extended beyond the scope of group-contribution methods by using problem-specific property models. At each design stage, novel optimization models and graph theoretic algorithms generate a large and diverse pool of candidates using an assortment of property models. The wide applicability and computational efficiency of the proposed methodology are illustrated through three case studies. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
A new framework to automate, augment, and accelerate steps in computer-aided molecular design is presented. The problem is tackled in three stages: (1) composition design, (2) structure determination, and (3) extended design. Composition identification and structure determination are decoupled to achieve computational efficiency. Using approximate group-contribution methods in the first stage, molecular compositions that fit design targets are identified. In the second stage, isomer structures of solution compositions are determined systematically, and structure-based property corrections are used to refine the solution pool. In the final stage, the design is extended beyond the scope of group-contribution methods by using problem-specific property models. At each design stage, novel optimization models and graph theoretic algorithms generate a large and diverse pool of candidates using an assortment of property models. The wide applicability and computational efficiency of the proposed methodology are illustrated through three case studies. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14111" xmlns="http://purl.org/rss/1.0/"><title>Capture of H2S from binary gas mixture by imidazolium-based ionic liquids with nonfluorous anions: A theoretical study</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14111</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Capture of H2S from binary gas mixture by imidazolium-based ionic liquids with nonfluorous anions: A theoretical study</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jie-Jie Chen, Wen-Wei Li, Han-Qing Yu, Xue-Liang Li</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-19T21:37:04.059814-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14111</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14111</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14111</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separations: Materials, Devices and 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Selective capture of H<sub>2</sub>S from gas mixture is essential to reduce its undesirable high corrosiveness and toxicity. Ionic liquids have been proposed as a promising material, and there is a need to clarify the capture mechanisms and search for optimal combination of cation and anion for application. This work aims to elucidate the interactions between H<sub>2</sub>S and nonfluorous imidazolium ionic liquids (NIILs) at a molecular level. The effects of hydroxyl group on the tail of alkyl chain, and combinations of imidazolium cations and nonfluorous anions on H<sub>2</sub>S capture are explored using quantum chemistry calculations. Furthermore, molecular dynamics simulations are used to explore the microstructural features of NIIL–H<sub>2</sub>S–CH<sub>4</sub> mixture systems. It is found that the hydroxyl groups in the cations is essential in governing the absorption properties of NIILs, including the interaction sites for hydrogen bonding, interaction geometries and energies, diffusion coefficients, and organization of H<sub>2</sub>S and CH<sub>4</sub> around cations and anions. A molecular viewpoint to design appropriate ionic liquids for promoting their applications for H<sub>2</sub>S capture is provided. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Selective capture of H2S from gas mixture is essential to reduce its undesirable high corrosiveness and toxicity. Ionic liquids have been proposed as a promising material, and there is a need to clarify the capture mechanisms and search for optimal combination of cation and anion for application. This work aims to elucidate the interactions between H2S and nonfluorous imidazolium ionic liquids (NIILs) at a molecular level. The effects of hydroxyl group on the tail of alkyl chain, and combinations of imidazolium cations and nonfluorous anions on H2S capture are explored using quantum chemistry calculations. Furthermore, molecular dynamics simulations are used to explore the microstructural features of NIIL–H2S–CH4 mixture systems. It is found that the hydroxyl groups in the cations is essential in governing the absorption properties of NIILs, including the interaction sites for hydrogen bonding, interaction geometries and energies, diffusion coefficients, and organization of H2S and CH4 around cations and anions. A molecular viewpoint to design appropriate ionic liquids for promoting their applications for H2S capture is provided. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14098" xmlns="http://purl.org/rss/1.0/"><title>Optimal design and operation of a steel plant integrated with a polygeneration system</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14098</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Optimal design and operation of a steel plant integrated with a polygeneration system</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hamid Ghanbari, Henrik Saxén, Ignacio E. Grossmann</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-19T20:42:43.163046-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14098</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14098</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14098</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A process integration approach has been applied to integrate a traditional steelmaking plant with a polygeneration system to increase energy efficiency and suppress carbon dioxide emissions from the system. Using short-cut models and empirical equations for different units and available technologies for gas separation, methane gasification, and methanol synthesis, a mixed integer nonlinear model is applied to find the optimal design of the polygeneration plant and operational conditions of the system. Due to the complexity of the blast furnace (BF) operation, a surrogate model technique is chosen based on an existing BF model. The results show that from an economic perspective, the pressure swing adsorption process with gas-phase methanol unit is preferred. The results demonstrate that integration of conventional steelmaking with a polygeneration system could decrease the specific emissions by more than 20 percent. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
A process integration approach has been applied to integrate a traditional steelmaking plant with a polygeneration system to increase energy efficiency and suppress carbon dioxide emissions from the system. Using short-cut models and empirical equations for different units and available technologies for gas separation, methane gasification, and methanol synthesis, a mixed integer nonlinear model is applied to find the optimal design of the polygeneration plant and operational conditions of the system. Due to the complexity of the blast furnace (BF) operation, a surrogate model technique is chosen based on an existing BF model. The results show that from an economic perspective, the pressure swing adsorption process with gas-phase methanol unit is preferred. The results demonstrate that integration of conventional steelmaking with a polygeneration system could decrease the specific emissions by more than 20 percent. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14108" xmlns="http://purl.org/rss/1.0/"><title>Insulin release dynamics from poly(diethylaminoethyl methacrylate) hydrogel systems</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14108</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Insulin release dynamics from poly(diethylaminoethyl methacrylate) hydrogel systems</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Steve R. Marek, Nicholas A. Peppas</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-19T15:21:29.876215-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14108</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14108</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14108</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Biomolecular Engineering, Bioengineering, Biochemicals, Biofuels, and Food</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Novel glucose-sensitive systems for the release of insulin from poly(diethylaminoethyl methacrylate) (PDEAEM) microparticles and nanoparticles decorated with glucose oxidase and catalase enzymes have been developed. The effect of polymer composition and loading conditions on the insulin loading efficiency and release was studied. The optimal conditions for loading insulin into PDEAEM microparticles were found to be at a loading pH of 5.6, particle to insulin mass ratio of 7:1, a concentration of 1.0 mg/mL insulin, and a collapsing pH of approximately 9.5. Microparticles exhibited a responsive (pH) or intelligent (glucose) release of insulin from a stimulus. Microparticles that had a nominal crosslinking ratio of 10% released a third of the insulin payload after a single stimulus, compared to nearly 70% for microparticles with a 3% crosslinking ratio. PDEAEM microparticles of 150 μm diameter showed promise as components of a system of automated, intelligent delivery method for insulin to type I diabetics. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Novel glucose-sensitive systems for the release of insulin from poly(diethylaminoethyl methacrylate) (PDEAEM) microparticles and nanoparticles decorated with glucose oxidase and catalase enzymes have been developed. The effect of polymer composition and loading conditions on the insulin loading efficiency and release was studied. The optimal conditions for loading insulin into PDEAEM microparticles were found to be at a loading pH of 5.6, particle to insulin mass ratio of 7:1, a concentration of 1.0 mg/mL insulin, and a collapsing pH of approximately 9.5. Microparticles exhibited a responsive (pH) or intelligent (glucose) release of insulin from a stimulus. Microparticles that had a nominal crosslinking ratio of 10% released a third of the insulin payload after a single stimulus, compared to nearly 70% for microparticles with a 3% crosslinking ratio. PDEAEM microparticles of 150 μm diameter showed promise as components of a system of automated, intelligent delivery method for insulin to type I diabetics. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14106" xmlns="http://purl.org/rss/1.0/"><title>Diffusion and performance of fragranced products: Prediction and validation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14106</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Diffusion and performance of fragranced products: Prediction and validation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Miguel A. Teixeira, Oscar Rodríguez, Alírio E. Rodrigues</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-19T15:12:30.206217-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14106</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14106</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14106</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena and Fluid Mechanics</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The design of fragranced products is a combination of art, technology, and scientific knowledge, although the former still predominates in the industry. For that reason, a theoretical model to assess their performance considering the release and diffusion together with the predicted odor intensity over time and distance from the source was developed and validated. Diffusion profiles were experimentally measured in a diffusion tube, similar to the Stefan tube, and predicted with a model for pure fragrance chemicals, binary, quaternary, and multicomponent (11 chemicals) mixtures. A very good agreement between our purely predictive model and experimental concentration data was observed. Fragrance concentrations in air were then converted into odor intensities using models from psychophysics, making it possible to evaluate the evolution of the odor with time and distance using a performance plot. Accordingly, the performance of these mixtures was modeled and experimentally validated, which constitutes a landmark for fragrance design. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The design of fragranced products is a combination of art, technology, and scientific knowledge, although the former still predominates in the industry. For that reason, a theoretical model to assess their performance considering the release and diffusion together with the predicted odor intensity over time and distance from the source was developed and validated. Diffusion profiles were experimentally measured in a diffusion tube, similar to the Stefan tube, and predicted with a model for pure fragrance chemicals, binary, quaternary, and multicomponent (11 chemicals) mixtures. A very good agreement between our purely predictive model and experimental concentration data was observed. Fragrance concentrations in air were then converted into odor intensities using models from psychophysics, making it possible to evaluate the evolution of the odor with time and distance using a performance plot. Accordingly, the performance of these mixtures was modeled and experimentally validated, which constitutes a landmark for fragrance design. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14104" xmlns="http://purl.org/rss/1.0/"><title>Adsorption of glucose into zeolite beta from aqueous solution</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14104</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Adsorption of glucose into zeolite beta from aqueous solution</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Peng Bai, J. Ilja Siepmann, Michael W. Deem</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-16T15:06:49.825664-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14104</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14104</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14104</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. Thermodynamics and Molecular-Scale 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Hydrophobic zeolites, including Ti- and Sn-beta, have been found to adsorb and isomerize glucose into fructose. An experimental question has been the significance of the entropic contribution to the free energy of transfer of glucose from solution to zeolite. We here perform Gibbs ensemble Monte Carlo calculations to quantify the enthalpy, entropy, and free energy of transfer of glucose from the aqueous phase to the zeolite phase. We find that the entropic contribution is large and positive, nearly compensating for an unfavorable enthalpy of transfer in all-silica zeolite beta. A significant component of the positive entropy of transfer from the aqueous phase to zeolite is the unstructuring of first coordination shell waters around glucose as it leaves the solution. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 00: 000–000, 2013</p></div>
]]></content:encoded><description>
Hydrophobic zeolites, including Ti- and Sn-beta, have been found to adsorb and isomerize glucose into fructose. An experimental question has been the significance of the entropic contribution to the free energy of transfer of glucose from solution to zeolite. We here perform Gibbs ensemble Monte Carlo calculations to quantify the enthalpy, entropy, and free energy of transfer of glucose from the aqueous phase to the zeolite phase. We find that the entropic contribution is large and positive, nearly compensating for an unfavorable enthalpy of transfer in all-silica zeolite beta. A significant component of the positive entropy of transfer from the aqueous phase to zeolite is the unstructuring of first coordination shell waters around glucose as it leaves the solution. © 2013 American Institute of Chemical Engineers AIChE J, 00: 000–000, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14091" xmlns="http://purl.org/rss/1.0/"><title>Ordered mesoporous carbons supported wacker-type catalyst for catalytic oxidative carbonylation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14091</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Ordered mesoporous carbons supported wacker-type catalyst for catalytic oxidative carbonylation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Bing Yan, Shouying Huang, Qingsen Meng, Yongli Shen, Shengping Wang, Xinbin Ma</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-15T10:01:43.751936-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14091</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14091</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14091</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Ordered mesoporous carbons (OMCs) were used as supports to prepare Wacker-type catalysts for diethyl carbonate (DEC) synthesis by oxidative carbonylation of ethanol in a gas-phase reaction. The effect of support structure on the dispersion of the active species and catalytic properties were investigated. Nitrogen sorption, X-ray diffraction (XRD) and transmission electron microscopy (TEM) results revealed that the active components have encapsulated in pore channels of OMCs. Characterizations of the catalysts, such as TEM, scanning electron microscope (SEM) and XRD, indicated that active components supported on OMCs have better dispersion compared to activated carbon (AC). The ethanol conversion of the catalysts was improved by ∼65% using OMCs as the catalyst support than AC. The stability of the catalytic activity can also be enhanced through surface modification of OMCs. Surface oxygen-containing groups (OCGs) on OMCs before and after surface modification were characterized by transmission IR spectra and the Beohm titration. The relationship between surface OCGs and anchor ability of OMCs was studied. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 00: 000–000, 2013</p></div>
]]></content:encoded><description>
Ordered mesoporous carbons (OMCs) were used as supports to prepare Wacker-type catalysts for diethyl carbonate (DEC) synthesis by oxidative carbonylation of ethanol in a gas-phase reaction. The effect of support structure on the dispersion of the active species and catalytic properties were investigated. Nitrogen sorption, X-ray diffraction (XRD) and transmission electron microscopy (TEM) results revealed that the active components have encapsulated in pore channels of OMCs. Characterizations of the catalysts, such as TEM, scanning electron microscope (SEM) and XRD, indicated that active components supported on OMCs have better dispersion compared to activated carbon (AC). The ethanol conversion of the catalysts was improved by ∼65% using OMCs as the catalyst support than AC. The stability of the catalytic activity can also be enhanced through surface modification of OMCs. Surface oxygen-containing groups (OCGs) on OMCs before and after surface modification were characterized by transmission IR spectra and the Beohm titration. The relationship between surface OCGs and anchor ability of OMCs was studied. © 2013 American Institute of Chemical Engineers AIChE J, 00: 000–000, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14102" xmlns="http://purl.org/rss/1.0/"><title>A composite equation of state for the modeling of sonic carbon dioxide jets in carbon capture and storage scenarios</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14102</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A composite equation of state for the modeling of sonic carbon dioxide jets in carbon capture and storage scenarios</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Christopher J. Wareing, Robert M. Woolley, Michael Fairweather, Samuel A. E. G. Falle</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-15T09:56:23.728748-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14102</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14102</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14102</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena and Fluid Mechanics</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The development of a novel composite two-phase method to predict the thermodynamic physical properties of carbon dioxide (CO<sub>2</sub>) above and below the triple point, applied herein in the context of Reynolds-Averaged Navier–Stokes computational modeling has been detailed here. A number of approaches have been combined to make accurate predictions in all three phases (solid, liquid, and gas) and at all phase changes for application in the modeling of releases of CO<sub>2</sub> at high pressure into the atmosphere. Predictions of a free release of CO<sub>2</sub> into the atmosphere from a reservoir at a pressure of 10 MPa and a temperature of 283 K, typical of transport conditions in carbon capture and storage scenarios, is examined. A comparison of the results shows that the sonic CO<sub>2</sub> jet that forms requires a three-phase equation of state including the latent heat of fusion to realistically simulate its characteristics. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 00: 000–000, 2013</p></div>
]]></content:encoded><description>
The development of a novel composite two-phase method to predict the thermodynamic physical properties of carbon dioxide (CO2) above and below the triple point, applied herein in the context of Reynolds-Averaged Navier–Stokes computational modeling has been detailed here. A number of approaches have been combined to make accurate predictions in all three phases (solid, liquid, and gas) and at all phase changes for application in the modeling of releases of CO2 at high pressure into the atmosphere. Predictions of a free release of CO2 into the atmosphere from a reservoir at a pressure of 10 MPa and a temperature of 283 K, typical of transport conditions in carbon capture and storage scenarios, is examined. A comparison of the results shows that the sonic CO2 jet that forms requires a three-phase equation of state including the latent heat of fusion to realistically simulate its characteristics. © 2013 American Institute of Chemical Engineers AIChE J, 00: 000–000, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14101" xmlns="http://purl.org/rss/1.0/"><title>Efficient scheduling method of complex batch processes with general network structure via agent-based modeling</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14101</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Efficient scheduling method of complex batch processes with general network structure via agent-based modeling</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yunfei Chu, John M. Wassick, Fengqi You</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-15T09:09:03.773411-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14101</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14101</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14101</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A novel efficient agent-based method for scheduling network batch processes in the process industry is proposed. The agent-based model is based on the resource-task network. To overcome the drawback of localized solutions found in conventional agent-based methods, a new scheduling algorithm is proposed. The algorithm predicts the objective function value by simulating another cloned agent-based model. Global information is obtained, and the solution quality is improved. The solution quality of this approach is validated by detailed comparisons with the mixed-integer programming (MIP) methods. A solution close to the optimal one can be found by the agent-based method with a much shorter computational time than the MIP methods. As a scheduling problem becomes increasingly complicated with increased scale, more specifications, and uncertainties, the advantages of the agent-based method become more evident. The proposed method is applied to simulated industrial problems where the MIP methods require excessive computational resources. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 00: 000–000, 2013</p></div>
]]></content:encoded><description>
A novel efficient agent-based method for scheduling network batch processes in the process industry is proposed. The agent-based model is based on the resource-task network. To overcome the drawback of localized solutions found in conventional agent-based methods, a new scheduling algorithm is proposed. The algorithm predicts the objective function value by simulating another cloned agent-based model. Global information is obtained, and the solution quality is improved. The solution quality of this approach is validated by detailed comparisons with the mixed-integer programming (MIP) methods. A solution close to the optimal one can be found by the agent-based method with a much shorter computational time than the MIP methods. As a scheduling problem becomes increasingly complicated with increased scale, more specifications, and uncertainties, the advantages of the agent-based method become more evident. The proposed method is applied to simulated industrial problems where the MIP methods require excessive computational resources. © 2013 American Institute of Chemical Engineers AIChE J, 00: 000–000, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14040" xmlns="http://purl.org/rss/1.0/"><title>Simultaneous process synthesis and control design under uncertainty: A worst-case performance approach</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14040</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Simultaneous process synthesis and control design under uncertainty: A worst-case performance approach</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Kelvyn Sánchez-Sánchez, Luis Ricardez-Sandoval</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-12T21:09:49.778192-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14040</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14040</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14040</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A new methodology that includes process synthesis and control structure decisions for the optimal process and control design of dynamic systems under uncertainty is presented. The method integrates dynamic flexibility and dynamic feasibility in a single optimization formulation, thus, reducing the costs to assess the optimal design. A robust stability test is also included in the proposed method to ensure that the optimal design is stable in the presence of magnitude-bounded perturbations. Since disturbances are treated as stochastic time-discrete unmeasured inputs, the optimal process synthesis and control design specified by this method remains feasible and stable in the presence of the most critical realizations in the disturbances. The proposed methodology has been applied to simultaneously design and control a system of CSTRs and a ternary distillation column. A study on the computational costs associated with this method is presented and compared to that required by a dynamic optimization-based scheme. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 00: 000–000, 2013</p></div>
]]></content:encoded><description>
A new methodology that includes process synthesis and control structure decisions for the optimal process and control design of dynamic systems under uncertainty is presented. The method integrates dynamic flexibility and dynamic feasibility in a single optimization formulation, thus, reducing the costs to assess the optimal design. A robust stability test is also included in the proposed method to ensure that the optimal design is stable in the presence of magnitude-bounded perturbations. Since disturbances are treated as stochastic time-discrete unmeasured inputs, the optimal process synthesis and control design specified by this method remains feasible and stable in the presence of the most critical realizations in the disturbances. The proposed methodology has been applied to simultaneously design and control a system of CSTRs and a ternary distillation column. A study on the computational costs associated with this method is presented and compared to that required by a dynamic optimization-based scheme. © 2013 American Institute of Chemical Engineers AIChE J, 00: 000–000, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14100" xmlns="http://purl.org/rss/1.0/"><title>A Stochastic Optimization approach for the design of Individualized Dosage Regimens</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14100</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A Stochastic Optimization approach for the design of Individualized Dosage Regimens</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">José M. Laínez-Aguirre, Gintaras V. Reklaitis</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-12T21:03:36.771966-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14100</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14100</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14100</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Quantitative methods for individualizing and optimizing the dosage regimen and clinically monitoring each patient are desirable to insure that each patient can obtain effective therapeutic benefit while minimizing undesirable side effects. This is of special concern for medicines that are expensive or whose toxic side effects are severe (e.g., oncological agents). The optimal dosage regimen for an individual is a combination of dose amount and/or dosing interval (i.e., time between doses) which minimizes the risk that the drug exposure deviates from the desired therapeutic window. The therapeutic window is defined as the range of drug exposure (e.g., blood concentration, area under the curve concentration-time) which is below a threshold defining an acceptable toxic side effect and above a threshold defining a minimum acceptable level of therapeutic efficacy. In this work, the dosage regimen optimization problem defined in terms of general pharmacometric models (i.e., described by differential-algebraic equations) is presented and a solution approach outlined which uses a scenario-based stochastic optimization formulation that minimizes a risk metric. The scenarios are derived from the posterior joint probability distribution of the individual's pharmacometric parameters which is obtained following an approximate Bayesian inference approach. A Smolyak rule is used for the selection of the scenarios (i.e., combination of pharmacometric parameters) to be considered and for computing the approximation to the risk metric. Two case studies, gabapentin and cyclophosphamide, are presented to elucidate the advantages and limitations of the proposed approach. The numerical results demonstrate that low risk optimal solutions can be generated via the proposed stochastic optimization; while significantly reducing the computational burden in comparison with the conventional Markov chain Monte Carlo—grid search approach. This partially alleviates implementation issues preventing the deployment of dosage regimen individualization in clinical practice. Since stochastic optimization has been extensively used in other domains, the approach for uncertainty characterization proposed in this work may have general relevance beyond the pharmacometrics domain. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 00: 000–000, 2013</p></div>
]]></content:encoded><description>
Quantitative methods for individualizing and optimizing the dosage regimen and clinically monitoring each patient are desirable to insure that each patient can obtain effective therapeutic benefit while minimizing undesirable side effects. This is of special concern for medicines that are expensive or whose toxic side effects are severe (e.g., oncological agents). The optimal dosage regimen for an individual is a combination of dose amount and/or dosing interval (i.e., time between doses) which minimizes the risk that the drug exposure deviates from the desired therapeutic window. The therapeutic window is defined as the range of drug exposure (e.g., blood concentration, area under the curve concentration-time) which is below a threshold defining an acceptable toxic side effect and above a threshold defining a minimum acceptable level of therapeutic efficacy. In this work, the dosage regimen optimization problem defined in terms of general pharmacometric models (i.e., described by differential-algebraic equations) is presented and a solution approach outlined which uses a scenario-based stochastic optimization formulation that minimizes a risk metric. The scenarios are derived from the posterior joint probability distribution of the individual's pharmacometric parameters which is obtained following an approximate Bayesian inference approach. A Smolyak rule is used for the selection of the scenarios (i.e., combination of pharmacometric parameters) to be considered and for computing the approximation to the risk metric. Two case studies, gabapentin and cyclophosphamide, are presented to elucidate the advantages and limitations of the proposed approach. The numerical results demonstrate that low risk optimal solutions can be generated via the proposed stochastic optimization; while significantly reducing the computational burden in comparison with the conventional Markov chain Monte Carlo—grid search approach. This partially alleviates implementation issues preventing the deployment of dosage regimen individualization in clinical practice. Since stochastic optimization has been extensively used in other domains, the approach for uncertainty characterization proposed in this work may have general relevance beyond the pharmacometrics domain. © 2013 American Institute of Chemical Engineers AIChE J, 00: 000–000, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14097" xmlns="http://purl.org/rss/1.0/"><title>Spectral properties and low-dimensional description of loop and recycle reactors</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14097</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Spectral properties and low-dimensional description of loop and recycle reactors</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Imran Alam, Vemuri Balakotaiah</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-08T11:07:49.169972-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14097</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14097</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14097</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. Reaction Engineering, 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The spectral properties of the discrete and continuous convection and convection-diffusion operators with loop or recycle boundary condition are analyzed. It is shown that the spectral properties of these nonsymmetric operators are closely related to the theory of circulant (Toeplitz) matrices and the complex Fourier series, respectively. Although there may be many complex eigenvalues, the smallest eigenvalue is real and approaches zero as the loop circulation or recycle ratio increases. This property is used to simplify nonlinear diffusion-convection-reaction models of loop and recycle reactors to obtain two-mode low-dimensional averaged models that are accurate in the limit of large recycle ratio. Explicit expressions for the two mixing coefficients that relate the two concentration modes and their dependence on various inlet conditions are also derived. Finally, the application of the low-dimensional models to determine the impact of macromixing on the conversion, yield, and selectivity for the case of nonlinear kinetics is illustrated. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The spectral properties of the discrete and continuous convection and convection-diffusion operators with loop or recycle boundary condition are analyzed. It is shown that the spectral properties of these nonsymmetric operators are closely related to the theory of circulant (Toeplitz) matrices and the complex Fourier series, respectively. Although there may be many complex eigenvalues, the smallest eigenvalue is real and approaches zero as the loop circulation or recycle ratio increases. This property is used to simplify nonlinear diffusion-convection-reaction models of loop and recycle reactors to obtain two-mode low-dimensional averaged models that are accurate in the limit of large recycle ratio. Explicit expressions for the two mixing coefficients that relate the two concentration modes and their dependence on various inlet conditions are also derived. Finally, the application of the low-dimensional models to determine the impact of macromixing on the conversion, yield, and selectivity for the case of nonlinear kinetics is illustrated. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14095" xmlns="http://purl.org/rss/1.0/"><title>Modeling and simulation of conditionally volume averaged viscoelastic two-phase flows</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14095</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Modeling and simulation of conditionally volume averaged viscoelastic two-phase flows</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Florian Habla, Laura Dietsche, Kai-Olaf Hinrichsen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-02T19:12:30.731383-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14095</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14095</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14095</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena and Fluid Mechanics</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Conditional volume averaging is used to develop a model capable of simulating two-phase flows of viscoelastic fluids with surface tension effects. The study is started with the single-phase mass and momentum balances, which are subsequently conditionally volume averaged. In doing so, In doing so, we arrive at a set of equations having unclosed interfacial terms, for which closure relations for viscoelastic fluids are presented. The resulting equations possess a structure similar to the single-phase equations; however, separate conservation equations are solved for each phase. As a result, each phase has its own pressure and velocity over the entire domain. Next, our numerical implementation is briefly outlined. We find that a Poiseuille single-phase flow is predicted correctly. The closure terms are examined by considering a two-phase shearing flow and a quiescient cylinder with surface tension. A convergence analysis is performed for a steady stratified two-phase flow with both phases being viscoelastic. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Conditional volume averaging is used to develop a model capable of simulating two-phase flows of viscoelastic fluids with surface tension effects. The study is started with the single-phase mass and momentum balances, which are subsequently conditionally volume averaged. In doing so, In doing so, we arrive at a set of equations having unclosed interfacial terms, for which closure relations for viscoelastic fluids are presented. The resulting equations possess a structure similar to the single-phase equations; however, separate conservation equations are solved for each phase. As a result, each phase has its own pressure and velocity over the entire domain. Next, our numerical implementation is briefly outlined. We find that a Poiseuille single-phase flow is predicted correctly. The closure terms are examined by considering a two-phase shearing flow and a quiescient cylinder with surface tension. A convergence analysis is performed for a steady stratified two-phase flow with both phases being viscoelastic. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14086" xmlns="http://purl.org/rss/1.0/"><title>Metabolic engineering of 2-petanone synthesis in Escherichia coli</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14086</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Metabolic engineering of 2-petanone synthesis in Escherichia coli</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ethan I. Lan, Yasumasa Dekishima, Derrick S. Chuang, James C. Liao</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-02T15:10:31.730189-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14086</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14086</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14086</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. Biomolecular Engineering, Bioengineering, Biofuels, and Food</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Expanding the chemical diversity of microbial fermentation products enables green production of fuel, chemicals, and pharmaceuticals. In recent years, coenzyme A (CoA) dependent chain elongation, resembling the reversed β-oxidation pathway, has attracted interest for its use in producing higher alcohols, fatty acids, and polyhydroxyalkanoate. To expand the chemical diversity of this pathway, we metabolically engineered Escherichia coli to produce 2-pentanone, which is not a natural fermentation product of E. coli. We describe the first demonstration of 2-pentanone synthesis in E. coli by coupling the CoA-dependent chain elongation with the acetone production pathway. By bioprospecting for enzymes capable of efficient hydrolysis of 3-keto-hexanoyl-CoA, production of 2-pentanone increased 20 fold, reaching a titer of 240 mg/L. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Expanding the chemical diversity of microbial fermentation products enables green production of fuel, chemicals, and pharmaceuticals. In recent years, coenzyme A (CoA) dependent chain elongation, resembling the reversed β-oxidation pathway, has attracted interest for its use in producing higher alcohols, fatty acids, and polyhydroxyalkanoate. To expand the chemical diversity of this pathway, we metabolically engineered Escherichia coli to produce 2-pentanone, which is not a natural fermentation product of E. coli. We describe the first demonstration of 2-pentanone synthesis in E. coli by coupling the CoA-dependent chain elongation with the acetone production pathway. By bioprospecting for enzymes capable of efficient hydrolysis of 3-keto-hexanoyl-CoA, production of 2-pentanone increased 20 fold, reaching a titer of 240 mg/L. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14096" xmlns="http://purl.org/rss/1.0/"><title>Numerical simulation of particle breakage in dry impact pulverizer</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14096</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Numerical simulation of particle breakage in dry impact pulverizer</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hirohisa Takeuchi, Hideya Nakamura, Satoru Watano</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-02T14:59:12.672462-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14096</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14096</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14096</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Particle Technology and Fluidization</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A novel method to simultaneously simulate particle motion and its breakage in a dry impact pulverizer was developed. The motion of particles in the pulverizer was calculated using a discrete phase model (DPM)-computational fluid dynamics (CFD) coupling model. When the particle impacts against a vessel wall, impact stress acting on the particle is calculated from Hertz's theory as a function of the impact velocity. At the same time, the particle strength as a function of the particle size is calculated from Griffith's theory. If the impact stress is larger than the particle strength, the particle is broken and replaced with smaller fragments. The size distribution of the fragments is obtained from a breakage function proposed. The motion of the fragments is calculated again by using the DPM-CFD coupling model. By repeating the above calculations over the whole particles, the grinding phenomenon can be simulated. The calculated results showed good agreement with the experimental one, and validity of the proposed method was confirmed. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
A novel method to simultaneously simulate particle motion and its breakage in a dry impact pulverizer was developed. The motion of particles in the pulverizer was calculated using a discrete phase model (DPM)-computational fluid dynamics (CFD) coupling model. When the particle impacts against a vessel wall, impact stress acting on the particle is calculated from Hertz's theory as a function of the impact velocity. At the same time, the particle strength as a function of the particle size is calculated from Griffith's theory. If the impact stress is larger than the particle strength, the particle is broken and replaced with smaller fragments. The size distribution of the fragments is obtained from a breakage function proposed. The motion of the fragments is calculated again by using the DPM-CFD coupling model. By repeating the above calculations over the whole particles, the grinding phenomenon can be simulated. The calculated results showed good agreement with the experimental one, and validity of the proposed method was confirmed. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14071" xmlns="http://purl.org/rss/1.0/"><title>Optimal engineered algae composition for the integrated simultaneous production of bioethanol and biodiesel</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14071</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Optimal engineered algae composition for the integrated simultaneous production of bioethanol and biodiesel</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mariano Martín, Ignacio E. Grossmann</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-02T09:20:23.188869-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14071</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14071</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14071</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The optimization of the composition of the algae for the simultaneous production of bioethanol and biodiesel is presented. We consider two alternative technologies for the biodiesel synthesis from algae oil, enzymatic or homogeneous alkali catalyzed that are coupled with bioethanol production from algae starch. In order to determine the optimal operating conditions, we not only couple the technologies, but simultaneously optimize the production of both biofuels and heat integrate them while optimizing the water consumption. Multi-effect distillation is included to reduce the energy and cooling water consumption for ethanol dehydration. In both cases, the optimal algae composition results in 60% oil, 30% starch, and 10% protein. The best alternative for the production of biofuels corresponds to a production price of 0.35 $/gal, using enzymes, with energy and water consumption values (4.00 MJ/gal and 0.59 gal/gal). © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The optimization of the composition of the algae for the simultaneous production of bioethanol and biodiesel is presented. We consider two alternative technologies for the biodiesel synthesis from algae oil, enzymatic or homogeneous alkali catalyzed that are coupled with bioethanol production from algae starch. In order to determine the optimal operating conditions, we not only couple the technologies, but simultaneously optimize the production of both biofuels and heat integrate them while optimizing the water consumption. Multi-effect distillation is included to reduce the energy and cooling water consumption for ethanol dehydration. In both cases, the optimal algae composition results in 60% oil, 30% starch, and 10% protein. The best alternative for the production of biofuels corresponds to a production price of 0.35 $/gal, using enzymes, with energy and water consumption values (4.00 MJ/gal and 0.59 gal/gal). © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14055" xmlns="http://purl.org/rss/1.0/"><title>Molecular insights for the optimization of solvent-based selective extraction of ethanol from fermentation broths</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14055</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Molecular insights for the optimization of solvent-based selective extraction of ethanol from fermentation broths</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Samuel J. Keasler, John L. Lewin, J. Ilja Siepmann, Nicole M. Gryska, Richard B. Ross, Nathan E. Schultz, Masayuki Nakamura</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-01T14:01:20.355653-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14055</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14055</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14055</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Thermodynamics and Molecular-Scale 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Simulations and experiments were carried out to explore the solvent extraction of ethanol from aqueous solution using a series of seven 10-carbon alcohols. It is shown that configurational-bias Monte Carlo simulations in the Gibbs ensemble coupled with the TraPPE-UA force field can be utilized for predictive screening of the different extraction abilities (in terms of capacity factor and selectivity) of these alcohols. Analysis of the simulation trajectories indicates that extraction capacity is connected to the stabilization of larger ethanol/water cluster in the organic solvent, whereas selectivity is improved when smaller ethanol/water clusters are more prevalent. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Simulations and experiments were carried out to explore the solvent extraction of ethanol from aqueous solution using a series of seven 10-carbon alcohols. It is shown that configurational-bias Monte Carlo simulations in the Gibbs ensemble coupled with the TraPPE-UA force field can be utilized for predictive screening of the different extraction abilities (in terms of capacity factor and selectivity) of these alcohols. Analysis of the simulation trajectories indicates that extraction capacity is connected to the stabilization of larger ethanol/water cluster in the organic solvent, whereas selectivity is improved when smaller ethanol/water clusters are more prevalent. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14061" xmlns="http://purl.org/rss/1.0/"><title>Sensitivity analyses for scenario reduction in flexible flow sheet design with a large number of uncertain parameters</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14061</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Sensitivity analyses for scenario reduction in flexible flow sheet design with a large number of uncertain parameters</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Zorka Novak Pintarič, Mihael Kasaš, Zdravko Kravanja</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-28T21:12:57.859508-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14061</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14061</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14061</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A solution strategy for designing flexible process flow sheets with a large number of uncertain parameters is presented. The basic mathematical formulation is a two-stage stochastic program transformed into its multi-scenario deterministic equivalent. The main feature of the proposed approach is a tremendous reduction in scenarios to a smaller number of those critical ones. This reduction is achieved through simple sensitivity analyses that identify those uncertain parameters that are critical for feasibility and those that are involved in a stochastic approximation of the objective value. Through the application of this strategy, it is possible to solve the problems with several tens or even hundred uncertain parameters, assuming weak interactions between them. Feasible designs are obtained for a fixed degree of flexibility, while the expected objective function is approximated fairly well. The strategy is applied to two flow sheet examples. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
A solution strategy for designing flexible process flow sheets with a large number of uncertain parameters is presented. The basic mathematical formulation is a two-stage stochastic program transformed into its multi-scenario deterministic equivalent. The main feature of the proposed approach is a tremendous reduction in scenarios to a smaller number of those critical ones. This reduction is achieved through simple sensitivity analyses that identify those uncertain parameters that are critical for feasibility and those that are involved in a stochastic approximation of the objective value. Through the application of this strategy, it is possible to solve the problems with several tens or even hundred uncertain parameters, assuming weak interactions between them. Feasible designs are obtained for a fixed degree of flexibility, while the expected objective function is approximated fairly well. The strategy is applied to two flow sheet examples. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14081" xmlns="http://purl.org/rss/1.0/"><title>Screening ionic liquids as candidates for separation of acid gases: Solubility of hydrogen sulfide, methane, and ethane</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14081</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Screening ionic liquids as candidates for separation of acid gases: Solubility of hydrogen sulfide, methane, and ethane</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Soheil Mortazavi-Manesh, Marco A. Satyro, Robert A. Marriott</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-28T09:14:08.521507-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14081</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14081</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14081</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separations: Materials, Devices and 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The solubility of the major constituents of natural gas in ionic liquids (ILs) can be used to identify their potential for acid gas removal from a producing gas stream. We have developed models for the solubility of H<sub>2</sub>S, CH<sub>4</sub>, and C<sub>2</sub>H<sub>6</sub> in ILs at typical conditions encountered in natural gas treatment. In this work, a conductor-like screening model for realistic solvation was used to predict the activity coefficients for solutes in ILs and a cubic EOS was used for vapor-phase corrections from ideality. Empirical correlations were developed to extrapolate solubilities where experimental data are not available at desired conditions; targeted in this study at 298.15 K and 2000 kPa. Over 400 possible ILs were ranked based on the higher selectivity of absorption of CO<sub>2</sub> and H<sub>2</sub>S over CH<sub>4</sub> and C<sub>2</sub>H<sub>6</sub>. The best 15% (58) of promising ILs for sour gas treatment predominantly contain the anions BF<sub>4</sub>, NO<sub>3</sub>, and CH<sub>3</sub>SO<sub>4</sub> and the cations N<sub>4111</sub>, pmg, and tmg. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The solubility of the major constituents of natural gas in ionic liquids (ILs) can be used to identify their potential for acid gas removal from a producing gas stream. We have developed models for the solubility of H2S, CH4, and C2H6 in ILs at typical conditions encountered in natural gas treatment. In this work, a conductor-like screening model for realistic solvation was used to predict the activity coefficients for solutes in ILs and a cubic EOS was used for vapor-phase corrections from ideality. Empirical correlations were developed to extrapolate solubilities where experimental data are not available at desired conditions; targeted in this study at 298.15 K and 2000 kPa. Over 400 possible ILs were ranked based on the higher selectivity of absorption of CO2 and H2S over CH4 and C2H6. The best 15% (58) of promising ILs for sour gas treatment predominantly contain the anions BF4, NO3, and CH3SO4 and the cations N4111, pmg, and tmg. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14063" xmlns="http://purl.org/rss/1.0/"><title>Data-driven model predictive quality control of batch processes</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14063</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Data-driven model predictive quality control of batch processes</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Siam Aumi, Brandon Corbett, Tracy Clarke-Pringle, Prashant Mhaskar</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-27T09:53:44.636245-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14063</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14063</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14063</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The problem of driving a batch process to a specified product quality using data-driven model predictive control (MPC) is described. To address the problem of unavailability of online quality measurements, an inferential quality model, which relates the process conditions over the entire batch duration to the final quality, is required. The accuracy of this type of quality model, however, is sensitive to the prediction of the future batch behavior until batch termination. In this work, we handle this “missing data” problem by integrating a previously developed data-driven modeling methodology, which combines multiple local linear models with an appropriate weighting function to describe nonlinearities, with the inferential model in a MPC framework. The key feature of this approach is that the causality and nonlinear relationships between the future inputs and outputs are accounted for in predicting the final quality and computing the manipulated input trajectory. The efficacy of the proposed predictive control design is illustrated via closed-loop simulations of a nylon-6,6 batch polymerization process with limited measurements. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The problem of driving a batch process to a specified product quality using data-driven model predictive control (MPC) is described. To address the problem of unavailability of online quality measurements, an inferential quality model, which relates the process conditions over the entire batch duration to the final quality, is required. The accuracy of this type of quality model, however, is sensitive to the prediction of the future batch behavior until batch termination. In this work, we handle this “missing data” problem by integrating a previously developed data-driven modeling methodology, which combines multiple local linear models with an appropriate weighting function to describe nonlinearities, with the inferential model in a MPC framework. The key feature of this approach is that the causality and nonlinear relationships between the future inputs and outputs are accounted for in predicting the final quality and computing the manipulated input trajectory. The efficacy of the proposed predictive control design is illustrated via closed-loop simulations of a nylon-6,6 batch polymerization process with limited measurements. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14084" xmlns="http://purl.org/rss/1.0/"><title>Minimal perfusion flow for osteogenic growth of mesenchymal stem cells on lattice scaffolds</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14084</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Minimal perfusion flow for osteogenic growth of mesenchymal stem cells on lattice scaffolds</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Marina Campolo, Francesco Curcio, Alfredo Soldati</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-26T12:11:03.904566-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14084</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14084</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14084</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena and Fluid Mechanics</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A modeling approach to identify sets of culture conditions to promote homogeneous growth of cells in perfusion bioreactors equipped with regular shape scaffolds is proposed. We identify cases in which dynamic culturing is necessary using a zero-dimensional mass transport and reaction model. Then, based on the three-dimensional (3-D) rendering of the flow field inside the bioreactor, we identify regions where cellular growth may become critical; finally, using a 1-D mass transport and reaction model, we calculate the minimal perfusion flow necessary to maintain the cellular growth rate above a target threshold. The developed approach is used to analyze culturing conditions inside an indirect perfusion bioreactor equipped with a lattice scaffold. Regions where the perfusion flow is inadequate to foster cellular growth at the desired rate are identified. The perfusion flow required to maintain the target growth rate inside the bioreactor is calculated. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
A modeling approach to identify sets of culture conditions to promote homogeneous growth of cells in perfusion bioreactors equipped with regular shape scaffolds is proposed. We identify cases in which dynamic culturing is necessary using a zero-dimensional mass transport and reaction model. Then, based on the three-dimensional (3-D) rendering of the flow field inside the bioreactor, we identify regions where cellular growth may become critical; finally, using a 1-D mass transport and reaction model, we calculate the minimal perfusion flow necessary to maintain the cellular growth rate above a target threshold. The developed approach is used to analyze culturing conditions inside an indirect perfusion bioreactor equipped with a lattice scaffold. Regions where the perfusion flow is inadequate to foster cellular growth at the desired rate are identified. The perfusion flow required to maintain the target growth rate inside the bioreactor is calculated. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14087" xmlns="http://purl.org/rss/1.0/"><title>Hydrodynamic separation of particles using pinched-flow fractionation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14087</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Hydrodynamic separation of particles using pinched-flow fractionation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">John F. Ashley, Christopher N. Bowman, Robert H. Davis</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-26T11:44:25.640556-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14087</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14087</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14087</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. Separations: Materials, Devices and 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Rigid particles transported through a pinched-flow fractionation (PFF) device are simulated using boundary-integral methods (BIM). The PFF device separates particles by size using a bifurcated microfluidic channel. The critical flow ratio of the two input channels required to achieve complete separation of large and small particles decreases with increasing diameter of the larger particles relative to the pinch height, and is nearly independent of the smaller particle size. A narrow pinch with a square exit was shown to have the lowest critical flow ratio and was selected as the model device to be fabricated. Experiments conducted using this device confirm that the larger particles exit further from the top wall than do the smaller particles, due to steric exclusion, and the final exit positions are within a few percent of the simulation results. It is shown that BIM is a valuable tool in the design of microfluidic devices. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Rigid particles transported through a pinched-flow fractionation (PFF) device are simulated using boundary-integral methods (BIM). The PFF device separates particles by size using a bifurcated microfluidic channel. The critical flow ratio of the two input channels required to achieve complete separation of large and small particles decreases with increasing diameter of the larger particles relative to the pinch height, and is nearly independent of the smaller particle size. A narrow pinch with a square exit was shown to have the lowest critical flow ratio and was selected as the model device to be fabricated. Experiments conducted using this device confirm that the larger particles exit further from the top wall than do the smaller particles, due to steric exclusion, and the final exit positions are within a few percent of the simulation results. It is shown that BIM is a valuable tool in the design of microfluidic devices. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14089" xmlns="http://purl.org/rss/1.0/"><title>Stochastic approach for the prediction of PSD in nonisothermal antisolvent crystallization processes</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14089</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Stochastic approach for the prediction of PSD in nonisothermal antisolvent crystallization processes</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Giuseppe Cogoni, Stefania Tronci, Giuseppe Mistretta, Roberto Baratti, Jose A. Romagnoli</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-26T11:20:40.287278-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14089</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14089</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14089</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A stochastic formulation for the description of cooling-antisolvent mediated crystal growth processes based on the Fokker-Planck equation is discussed. Previous results are further extended to include not only the additional degree of freedom (temperature) in the approach, but also to formulate the model parameters dependencies with the input manipulated variables (antisolvent flow rate and temperature) toward a global model to be used within all possible operating regimes. The obtained global models are used to define, for the first time, an operating map of the crystallization process, where asymptotic isomean and isovariance curves are reported in an antisolvent flow-rate-temperature plane. Input multiplicities are identified and validated both numerically and experimentally for the NaCl-water-ethanol nonisothermal antisolvent crystallization system. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
A stochastic formulation for the description of cooling-antisolvent mediated crystal growth processes based on the Fokker-Planck equation is discussed. Previous results are further extended to include not only the additional degree of freedom (temperature) in the approach, but also to formulate the model parameters dependencies with the input manipulated variables (antisolvent flow rate and temperature) toward a global model to be used within all possible operating regimes. The obtained global models are used to define, for the first time, an operating map of the crystallization process, where asymptotic isomean and isovariance curves are reported in an antisolvent flow-rate-temperature plane. Input multiplicities are identified and validated both numerically and experimentally for the NaCl-water-ethanol nonisothermal antisolvent crystallization system. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14083" xmlns="http://purl.org/rss/1.0/"><title>A NIR luminescent copolymer based on platinum porphyrin as high permeable dissolved oxygen sensor for microbioreactors</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14083</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A NIR luminescent copolymer based on platinum porphyrin as high permeable dissolved oxygen sensor for microbioreactors</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Pengwei Jin, Ju Chu, Yu Miao, Jun Tan, Siliang Zhang, Weihong Zhu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-22T22:22:23.385885-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14083</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14083</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14083</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Biomolecular Engineering, Bioengineering, Biochemicals, Biofuels, and Food</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Microbioreactors with multioptical sensors have become increasingly important because of their small working volumes, high degree of parallelization and the available robotics. A novel hydrophobic luminescent copolymer P(Pt-TPP-TFEMA) along with reference P(Pt-TPP-EMA) containing the pendant group of 5,10,15,20-tetraphenylporphyrin (TPP) moiety as low-cost dissolved oxygen (DO) chemosensor film for high-throughput microbioreactors is designed. Its sensor film exhibits fast response to DO with good stability and fatigue resistance, being capable of applying as a low-cost DO indicator for high-throughput bioprocess measurement. Results show that the quenching response of DO increases with the enhancement in the copolymeric hydrophobicity using the presented hybrid fluorinated ethyl methacrylate. Furthermore, the long emission band at 650 nm of chromophore TPP with large Stoke's shift about 250 nm brings several advantages, such as low scattering, deep penetration, and minimal interferences of absorption and fluorescence from the fermentation system, which shows high-promising application in bioprocess monitoring. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Microbioreactors with multioptical sensors have become increasingly important because of their small working volumes, high degree of parallelization and the available robotics. A novel hydrophobic luminescent copolymer P(Pt-TPP-TFEMA) along with reference P(Pt-TPP-EMA) containing the pendant group of 5,10,15,20-tetraphenylporphyrin (TPP) moiety as low-cost dissolved oxygen (DO) chemosensor film for high-throughput microbioreactors is designed. Its sensor film exhibits fast response to DO with good stability and fatigue resistance, being capable of applying as a low-cost DO indicator for high-throughput bioprocess measurement. Results show that the quenching response of DO increases with the enhancement in the copolymeric hydrophobicity using the presented hybrid fluorinated ethyl methacrylate. Furthermore, the long emission band at 650 nm of chromophore TPP with large Stoke's shift about 250 nm brings several advantages, such as low scattering, deep penetration, and minimal interferences of absorption and fluorescence from the fermentation system, which shows high-promising application in bioprocess monitoring. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14068" xmlns="http://purl.org/rss/1.0/"><title>Acylation desulfurization of oil via reactive adsorption</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14068</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Acylation desulfurization of oil via reactive adsorption</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jiajun Gao, Xingyu Chen, Nannan Ren, Wenjiao Wu, Chunxi Li, Hong Meng, Yingzhou Lu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-20T20:33:45.351208-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14068</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14068</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14068</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separations: Materials, Devices and 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Excellent desulfurization is achieved via reactive adsorption using Friedel-Crafts acylation materials, that is, acylating reagents and Lewis acids, such as acetyl chloride (AC) and AlCl<sub>3</sub>, being named as acylation desulfurization (ACDS). For model oil, thiophenic compounds, namely, dibenzothiophene, benzothiophene, and thiophene, are removed completely by AC–AlCl<sub>3</sub> within 30 min at room temperature. In this process, thiophenic compounds are acylated by AC under the catalysis of AlCl<sub>3</sub>, and the acylated derivatives are stronger base than original ones due to incorporation of O-containing carbonyl group (C<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8fe.gif" alt="[DOUBLE BOND]"/>O) and, thus, adsorbed more easily by AlCl<sub>3</sub> via Lewis acid–base complexation. Further, ACDS mechanism is identified by acylated product characterization and quantum chemistry calculation. Satisfactorily, ACDS is still effective for toluene-rich and real oils, and real oil quality is improved with desulfurization proceeding. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Excellent desulfurization is achieved via reactive adsorption using Friedel-Crafts acylation materials, that is, acylating reagents and Lewis acids, such as acetyl chloride (AC) and AlCl3, being named as acylation desulfurization (ACDS). For model oil, thiophenic compounds, namely, dibenzothiophene, benzothiophene, and thiophene, are removed completely by AC–AlCl3 within 30 min at room temperature. In this process, thiophenic compounds are acylated by AC under the catalysis of AlCl3, and the acylated derivatives are stronger base than original ones due to incorporation of O-containing carbonyl group (C<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8fe.gif" alt="[DOUBLE BOND]"/>O) and, thus, adsorbed more easily by AlCl3 via Lewis acid–base complexation. Further, ACDS mechanism is identified by acylated product characterization and quantum chemistry calculation. Satisfactorily, ACDS is still effective for toluene-rich and real oils, and real oil quality is improved with desulfurization proceeding. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14070" xmlns="http://purl.org/rss/1.0/"><title>Vapor recompression for efficient distillation. 1. A new synthesis perspective on standard configurations</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14070</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Vapor recompression for efficient distillation. 1. A new synthesis perspective on standard configurations</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">N. Felbab, B. Patel, M. M. El-Halwagi, D. Hildebrandt, D. Glasser</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-20T20:33:38.986991-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14070</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14070</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14070</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separations: Materials, Devices and 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The vapor recompression (VRC) distillation scheme is examined and compared with conventional distillation in an analysis spanning fundamental thermodynamics, high-level calculations, and rigorous simulation. The purpose of this article is three-fold: first, it provides greater insight into VRC distillation. Second, it provides a process synthesis tool to rapidly assess whether VRC is likely to be more thermodynamically favorable than conventional distillation for a given split. Third, it may be used to determine if VRC can be implemented practically. The tool presented in the article is consolidated in the form of a single chart, for which only the top and bottom product temperatures are required to determine the outcome. Using this chart, first-pass estimates can be obtained with no calculations whatsoever. The tool, which appears to be the first of its kind in this context, is validated with examples and rigorous simulation. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The vapor recompression (VRC) distillation scheme is examined and compared with conventional distillation in an analysis spanning fundamental thermodynamics, high-level calculations, and rigorous simulation. The purpose of this article is three-fold: first, it provides greater insight into VRC distillation. Second, it provides a process synthesis tool to rapidly assess whether VRC is likely to be more thermodynamically favorable than conventional distillation for a given split. Third, it may be used to determine if VRC can be implemented practically. The tool presented in the article is consolidated in the form of a single chart, for which only the top and bottom product temperatures are required to determine the outcome. Using this chart, first-pass estimates can be obtained with no calculations whatsoever. The tool, which appears to be the first of its kind in this context, is validated with examples and rigorous simulation. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14024" xmlns="http://purl.org/rss/1.0/"><title>Mapping of regimes for the key processes in wet granulation: Foam vs. spray</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14024</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Mapping of regimes for the key processes in wet granulation: Foam vs. spray</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Melvin X.L. Tan, Karen P. Hapgood</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-20T00:49:41.653954-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14024</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14024</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14024</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Particle Technology and Fluidization</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The evaluation of foam and spray granulation mechanisms and their performances in achieving uniform liquid distribution in a high-shear mixer-granulator is presented. A regime map is presented to describe the granulation mechanisms for the foam and spray systems. Foam and spray granulation are shown to successfully create granules of well-distributed moisture at the end of wet massing despite there was a deviation from the theoretical moisture content at the end of binder addition. In the wetting and nucleation regime, spray granulation involves drop penetration nucleation outside of the drop-controlled regime, whereas foam granulation operates favorably in the mechanical dispersion regime. For foam granulation, mechanical dispersion produces more uniform granule-size distributions below the overwetting limit. Spray granulation exhibits steady granule growth, whereas foam granulation shows induction granule growth followed by rapid granule growth. The regime map provides a basis to customize formulations and compare the different foam and spray granulation mechanisms. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The evaluation of foam and spray granulation mechanisms and their performances in achieving uniform liquid distribution in a high-shear mixer-granulator is presented. A regime map is presented to describe the granulation mechanisms for the foam and spray systems. Foam and spray granulation are shown to successfully create granules of well-distributed moisture at the end of wet massing despite there was a deviation from the theoretical moisture content at the end of binder addition. In the wetting and nucleation regime, spray granulation involves drop penetration nucleation outside of the drop-controlled regime, whereas foam granulation operates favorably in the mechanical dispersion regime. For foam granulation, mechanical dispersion produces more uniform granule-size distributions below the overwetting limit. Spray granulation exhibits steady granule growth, whereas foam granulation shows induction granule growth followed by rapid granule growth. The regime map provides a basis to customize formulations and compare the different foam and spray granulation mechanisms. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14065" xmlns="http://purl.org/rss/1.0/"><title>Influence of formic acid on electrochemical properties of high-porosity Pt/TiN nanoparticle aggregates</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14065</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Influence of formic acid on electrochemical properties of high-porosity Pt/TiN nanoparticle aggregates</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Takashi Ogi, Ratna Balgis, Kikuo Okuyama, Naoko Tajima, Heru Setyawan</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-19T21:39:56.531581-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14065</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14065</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14065</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Inorganic Materials: Synthesis and Processing</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Platinum-deposited titanium nitride (Pt/TiN) nanoparticle aggregates with high porosities were successfully prepared via a self-assembly-assisted spray pyrolysis method. The addition of formic acid (HCOOH) had a significant influence on the process, promoting the simultaneous formation of metallic Pt and reduction on the surface of the TiN support material. Complete reduction of the Pt/TiN nanoparticle aggregates improved the catalytic activity. The electrochemical surface area (ECSA) of Pt/TiN with HCOOH (Pt/TiN<sub>w/HCOOH</sub>) was 87.15 m<sup>2</sup>/g-Pt, which was higher than that of Pt/TiN without HCOOH (Pt/TiN<sub>w/o-HCOOH</sub>). The catalytic durability of Pt/TiN<sub>w/HCOOH</sub> was twice that of Pt/TiN<sub>w/o-HCOOH</sub>. An effective strategy for obtaining carbon-free catalysts with high activities and durabilities was identified. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Platinum-deposited titanium nitride (Pt/TiN) nanoparticle aggregates with high porosities were successfully prepared via a self-assembly-assisted spray pyrolysis method. The addition of formic acid (HCOOH) had a significant influence on the process, promoting the simultaneous formation of metallic Pt and reduction on the surface of the TiN support material. Complete reduction of the Pt/TiN nanoparticle aggregates improved the catalytic activity. The electrochemical surface area (ECSA) of Pt/TiN with HCOOH (Pt/TiNw/HCOOH) was 87.15 m2/g-Pt, which was higher than that of Pt/TiN without HCOOH (Pt/TiNw/o-HCOOH). The catalytic durability of Pt/TiNw/HCOOH was twice that of Pt/TiNw/o-HCOOH. An effective strategy for obtaining carbon-free catalysts with high activities and durabilities was identified. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14080" xmlns="http://purl.org/rss/1.0/"><title>Convection battery—modeling, insight, and review</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14080</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Convection battery—modeling, insight, and review</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Michael Gordon, Galen Suppes</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-18T16:53:04.80506-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14080</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14080</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14080</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Porous electrode theory was used to model performance of the convection battery using lithium iron-phosphate chemistry. The model results and underlying equations were able to quantify and extend previous interpretations of laboratory validation studies. These analyses substantiated the following conclusions on the performance of the convection battery: (a) flow in the convection battery can reduce concentration overpotentials by 99.9%, (b) both the ionic and electron conductivities of solid phases can have a major impact on convection battery performance, and (c) the solid-phase ionic conductivity of a porous separator is an important design parameter and is not considered by porous electrode theory as published to date. In view of the ability of the convection battery to overcome both bulk diffusion and liquid-phase effective conductivity limitations; the convection battery has an unprecedented potential to redefine the performance of large batteries. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 00: 000–000, 2013</p></div>
]]></content:encoded><description>
Porous electrode theory was used to model performance of the convection battery using lithium iron-phosphate chemistry. The model results and underlying equations were able to quantify and extend previous interpretations of laboratory validation studies. These analyses substantiated the following conclusions on the performance of the convection battery: (a) flow in the convection battery can reduce concentration overpotentials by 99.9%, (b) both the ionic and electron conductivities of solid phases can have a major impact on convection battery performance, and (c) the solid-phase ionic conductivity of a porous separator is an important design parameter and is not considered by porous electrode theory as published to date. In view of the ability of the convection battery to overcome both bulk diffusion and liquid-phase effective conductivity limitations; the convection battery has an unprecedented potential to redefine the performance of large batteries. © 2013 American Institute of Chemical Engineers AIChE J, 00: 000–000, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14076" xmlns="http://purl.org/rss/1.0/"><title>Reducing total annualized cost and CO2 emissions in batch distillation: Dynamics and control</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14076</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Reducing total annualized cost and CO2 emissions in batch distillation: Dynamics and control</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Gara Uday Bhaskar Babu, Amiya K. Jana</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-17T14:18:59.143515-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14076</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14076</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14076</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>In this contribution, the direct vapor recompression approach is introduced in a batch distillation operated at an unsteady state condition. This vapor recompressed batch distillation (VRBD) accompanies an isentropic compressor that runs at a fixed as well as variable speed. Aiming to ensure the optimal use of internal heat source, an open-loop control policy is proposed for the VRBD that adjusts either the overhead vapor splitting or the external heat supply to the reboiler. Again, the variable speed VRBD additionally involves the manipulation of compression ratio. Developing two alternative configurations of VRBD column, the best heat integrated scheme is attempted to identify in the aspects of energy efficiency and total annualized cost for further advancement. A closed-loop control algorithm for the best performing variable speed VRBD aiming to meet the end objective of relatively high-purity product discharged at a constant composition is developed. The separation of a reactive system is considered to illustrate these results and demonstrate the effectiveness of the novel VRBD scheme. Performing simulation tests, it is investigated that the closed-loop control operation substantially improves not only the distillate purity but also the total amount of product. Achieving significant improvement in thermodynamic efficiency and cost by the controlled heat integrated scheme over its conventional counterpart, finally the attractiveness of the VRBD column by investigating its potential to reduce the greenhouse gas (i.e., CO<sub>2</sub>) emissions is shown. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
In this contribution, the direct vapor recompression approach is introduced in a batch distillation operated at an unsteady state condition. This vapor recompressed batch distillation (VRBD) accompanies an isentropic compressor that runs at a fixed as well as variable speed. Aiming to ensure the optimal use of internal heat source, an open-loop control policy is proposed for the VRBD that adjusts either the overhead vapor splitting or the external heat supply to the reboiler. Again, the variable speed VRBD additionally involves the manipulation of compression ratio. Developing two alternative configurations of VRBD column, the best heat integrated scheme is attempted to identify in the aspects of energy efficiency and total annualized cost for further advancement. A closed-loop control algorithm for the best performing variable speed VRBD aiming to meet the end objective of relatively high-purity product discharged at a constant composition is developed. The separation of a reactive system is considered to illustrate these results and demonstrate the effectiveness of the novel VRBD scheme. Performing simulation tests, it is investigated that the closed-loop control operation substantially improves not only the distillate purity but also the total amount of product. Achieving significant improvement in thermodynamic efficiency and cost by the controlled heat integrated scheme over its conventional counterpart, finally the attractiveness of the VRBD column by investigating its potential to reduce the greenhouse gas (i.e., CO2) emissions is shown. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14082" xmlns="http://purl.org/rss/1.0/"><title>A new multi-scale model based on CFD and macroscopic calculation for corrugated structured packing column</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14082</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A new multi-scale model based on CFD and macroscopic calculation for corrugated structured packing column</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">B. Sun, L. He, B.T. Liu, F. Gu, C.J. Liu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-16T18:08:17.685394-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14082</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14082</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14082</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena and Fluid Mechanics</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A multi-scale approach with the combination of computational fluid dynamic (CFD) and macroscopic calculation methods has been proposed to predict the hydrodynamics behavior in the corrugated structured packing column. On the basis of the concept of the representative unit, the three-dimensional (3-D) volume of fluid (VOF) model of the structured packing is applied in the small scale simulation, and the stream split fraction coefficients and effective wetted area ratio are calculated. The unit network model, which is a mechanistic model, is applied in large scale calculation basing on the small scale results. The liquid holdup distribution in the entire column can be available by this multi-scale method. A comparison between the simulation results and the experimental data of our previous work is given to validate the present model. The multi-scale model is proved to be prospective to assist the analysis and design of structure packing columns in chemical engineering. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
A multi-scale approach with the combination of computational fluid dynamic (CFD) and macroscopic calculation methods has been proposed to predict the hydrodynamics behavior in the corrugated structured packing column. On the basis of the concept of the representative unit, the three-dimensional (3-D) volume of fluid (VOF) model of the structured packing is applied in the small scale simulation, and the stream split fraction coefficients and effective wetted area ratio are calculated. The unit network model, which is a mechanistic model, is applied in large scale calculation basing on the small scale results. The liquid holdup distribution in the entire column can be available by this multi-scale method. A comparison between the simulation results and the experimental data of our previous work is given to validate the present model. The multi-scale model is proved to be prospective to assist the analysis and design of structure packing columns in chemical engineering. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14073" xmlns="http://purl.org/rss/1.0/"><title>Phase Evolution and Nature of Oxide Dissolution in Metallurgical Slags</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14073</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Phase Evolution and Nature of Oxide Dissolution in Metallurgical Slags</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Zhi H. I. Sun, Xiaoling Guo, Joris Dyck, Muxing Guo, Bart Blanpain</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-15T09:15:37.888464-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14073</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14073</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14073</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The dissolution of solid lime particles into liquid slags at high temperatures was evaluated by means of confocal scanning laser microscopy. An additional solid layer around the lime particle was observed at the intermediate stage of the dissolution into CaO<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>Al<sub>2</sub>O<sub>3</sub><img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>SiO<sub>2</sub> slags. The dissolution rate was decelerated due to the existence of the additional layer and the dissolution profile could be clearly distinguished into three stages, that is, an early, intermediate, and late stage. By adding 10 wt % MgO, this layer could be effectively eliminated and the slope of the whole dissolution profile kept relatively constant. The dissolution path and mechanisms were subsequently evaluated by incorporating thermodynamic calculations. Both direct and indirect dissolutions could be distinguished. It was realized that the decrease in composition range for solid precipitating after adding MgO could significantly reduce the interfacial reaction (IR) layer formation. Post-mortem analyses on quenched samples were further carried out to confirm the theoretical calculations. It was found that the solid layer in slags without MgO was (CaO)<sub>2</sub>·SiO<sub>2</sub> and (CaO)<sub>3</sub>·SiO<sub>2</sub> which is in line with the thermodynamic calculations. However, only (CaO)<sub>2</sub>·SiO<sub>2</sub> was noticed in slags with MgO which both (CaO)<sub>2</sub>·SiO<sub>2</sub> and MgO phases should be present according to the calculations. The nonequilibrium during dissolution may play an important role on phase transformation and MgO particles in much smaller quantity may have dissolved into (CaO)<sub>2</sub>·SiO<sub>2</sub> phase. The diffusion of CaO in both slags with and without MgO was additionally investigated. The local CaO concentration distributions from the direct dissolution phase to the slag bulk could be well fitted with the theoretical model proposed via Fick's second law. As a result, the local diffusion coefficient in the dissolution region was obtained and the effect of MgO addition on diffusion could be assessed. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 00: 000–000, 2013</p></div>
]]></content:encoded><description>
The dissolution of solid lime particles into liquid slags at high temperatures was evaluated by means of confocal scanning laser microscopy. An additional solid layer around the lime particle was observed at the intermediate stage of the dissolution into CaO<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>Al2O3<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>SiO2 slags. The dissolution rate was decelerated due to the existence of the additional layer and the dissolution profile could be clearly distinguished into three stages, that is, an early, intermediate, and late stage. By adding 10 wt % MgO, this layer could be effectively eliminated and the slope of the whole dissolution profile kept relatively constant. The dissolution path and mechanisms were subsequently evaluated by incorporating thermodynamic calculations. Both direct and indirect dissolutions could be distinguished. It was realized that the decrease in composition range for solid precipitating after adding MgO could significantly reduce the interfacial reaction (IR) layer formation. Post-mortem analyses on quenched samples were further carried out to confirm the theoretical calculations. It was found that the solid layer in slags without MgO was (CaO)2·SiO2 and (CaO)3·SiO2 which is in line with the thermodynamic calculations. However, only (CaO)2·SiO2 was noticed in slags with MgO which both (CaO)2·SiO2 and MgO phases should be present according to the calculations. The nonequilibrium during dissolution may play an important role on phase transformation and MgO particles in much smaller quantity may have dissolved into (CaO)2·SiO2 phase. The diffusion of CaO in both slags with and without MgO was additionally investigated. The local CaO concentration distributions from the direct dissolution phase to the slag bulk could be well fitted with the theoretical model proposed via Fick's second law. As a result, the local diffusion coefficient in the dissolution region was obtained and the effect of MgO addition on diffusion could be assessed. © 2013 American Institute of Chemical Engineers AIChE J, 00: 000–000, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14079" xmlns="http://purl.org/rss/1.0/"><title>Helical liquid flow on a vertical cylinder and its application to gas absorption</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14079</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Helical liquid flow on a vertical cylinder and its application to gas absorption</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Naoya Komae, Yuki Sato,, Yasuhiko H. Mori</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-14T09:22:08.166513-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14079</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14079</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14079</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport and Fluid Mechanics</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>An experimental examination of a novel device for enhancing the gas absorption into an aqueous absorbent flowing down the outer wall of a vertical cylinder was reported. This device utilizes flexible strings tightly wound around the cylinder, taking the form of a multiple helix. The absorbent flows along parallel channels partitioned by the strings, maintaining mutual contact with the surrounding gas for a longer time than it would when it flows down the same cylinder wall in the absence of such strings. Both flow-observation experiments and absorption experiments using water as the absorbent flowing along a single helical channel and carbon dioxide as the gas to be absorbed were carried out. The effectiveness of the helical-flow device for promoting the absorption was recognized at water flow rates high enough to induce an oscillatory flow mode accompanied by periodical liquid−gas interface deformation. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
An experimental examination of a novel device for enhancing the gas absorption into an aqueous absorbent flowing down the outer wall of a vertical cylinder was reported. This device utilizes flexible strings tightly wound around the cylinder, taking the form of a multiple helix. The absorbent flows along parallel channels partitioned by the strings, maintaining mutual contact with the surrounding gas for a longer time than it would when it flows down the same cylinder wall in the absence of such strings. Both flow-observation experiments and absorption experiments using water as the absorbent flowing along a single helical channel and carbon dioxide as the gas to be absorbed were carried out. The effectiveness of the helical-flow device for promoting the absorption was recognized at water flow rates high enough to induce an oscillatory flow mode accompanied by periodical liquid−gas interface deformation. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14072" xmlns="http://purl.org/rss/1.0/"><title>Efficient Capture of Carbon Dioxide with Novel Mass-Transfer Intensification Device Using Ionic Liquids</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14072</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Efficient Capture of Carbon Dioxide with Novel Mass-Transfer Intensification Device Using Ionic Liquids</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Liang-Liang Zhang, Jie-Xin Wang, Zhi-Ping Liu, Ying Lu, Guang-Wen Chu, Wen-Chuan Wang, Jian-Feng Chen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-14T08:30:36.054792-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14072</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14072</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14072</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separations: Materials, Devices and 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A novel mass-transfer intensified approach for CO<sub>2</sub> capture with ionic liquids (ILs) using rotating packed bed (RPB) reactor was presented. This new approach combined the advantages of RPB as a high mass-transfer intensification device for viscous system and IL as a novel, environmentally benign CO<sub>2</sub> capture media with high thermal stability and extremely low volatility. Amino-functionalized IL (2-hydroxyethyl)-trimethyl-ammonium (S)−2-pyrrolidinecarboxylic acid salt ([Choline][Pro]) was synthesized to perform experimental examination of CO<sub>2</sub> capture by chemical absorption. In RPB, it took only 0.2 s to reach 0.2 mol CO<sub>2</sub>/mol IL at 293 K, indicating that RPB was kinetically favorable to absorption of CO<sub>2</sub> in IL because of its efficient mass-transfer intensification. The effects of operation parameters on CO<sub>2</sub> removal efficiency and IL absorbent capacity were studied. In addition, a model based on penetration theory was proposed to explore the mechanism of gas–liquid mass transfer of ILs system in RPB. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 00: 000–000, 2013</p></div>
]]></content:encoded><description>
A novel mass-transfer intensified approach for CO2 capture with ionic liquids (ILs) using rotating packed bed (RPB) reactor was presented. This new approach combined the advantages of RPB as a high mass-transfer intensification device for viscous system and IL as a novel, environmentally benign CO2 capture media with high thermal stability and extremely low volatility. Amino-functionalized IL (2-hydroxyethyl)-trimethyl-ammonium (S)−2-pyrrolidinecarboxylic acid salt ([Choline][Pro]) was synthesized to perform experimental examination of CO2 capture by chemical absorption. In RPB, it took only 0.2 s to reach 0.2 mol CO2/mol IL at 293 K, indicating that RPB was kinetically favorable to absorption of CO2 in IL because of its efficient mass-transfer intensification. The effects of operation parameters on CO2 removal efficiency and IL absorbent capacity were studied. In addition, a model based on penetration theory was proposed to explore the mechanism of gas–liquid mass transfer of ILs system in RPB. © 2013 American Institute of Chemical Engineers AIChE J, 00: 000–000, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14064" xmlns="http://purl.org/rss/1.0/"><title>The Simplest Stirred Tank for Laminar Mixing: Mixing in a Vessel Agitated by an Off-Centered Angled Disc</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14064</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">The Simplest Stirred Tank for Laminar Mixing: Mixing in a Vessel Agitated by an Off-Centered Angled Disc</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">D. Bulnes-Abundis, M. M. Alvarez</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-14T07:43:22.181841-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14064</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14064</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14064</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena and Fluid Mechanics</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>We study the mixing structure, mixing performance, and short term dynamics in round bottomed laminar tanks agitated by an eccentrically located angled disc. We define eccentricity (E = e/R) as the ratio of the distance of the axis of rotation from the center line of the tank (e) and the tank radius (R). The structural and dynamic features observed at different eccentricity values were compared using planar laser-induced fluorescence techniques and computational fluid dynamics calculations. A Poincaré analysis demonstrates the chaotic nature of the flow induced by eccentricity. Practically globally chaotic conditions are observed for E = 0.42 and E = 0.50, with mixing times of 5–8 min at Re = 416. We study the effect of different injection points on the short-term mixing dynamics and we calculate axial flow rates and Power numbers. Stirred tanks agitated by an eccentrically located angled disc are a simple and cost effective system for laminar mixing applications. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 00: 000–000, 2013</p></div>
]]></content:encoded><description>
We study the mixing structure, mixing performance, and short term dynamics in round bottomed laminar tanks agitated by an eccentrically located angled disc. We define eccentricity (E = e/R) as the ratio of the distance of the axis of rotation from the center line of the tank (e) and the tank radius (R). The structural and dynamic features observed at different eccentricity values were compared using planar laser-induced fluorescence techniques and computational fluid dynamics calculations. A Poincaré analysis demonstrates the chaotic nature of the flow induced by eccentricity. Practically globally chaotic conditions are observed for E = 0.42 and E = 0.50, with mixing times of 5–8 min at Re = 416. We study the effect of different injection points on the short-term mixing dynamics and we calculate axial flow rates and Power numbers. Stirred tanks agitated by an eccentrically located angled disc are a simple and cost effective system for laminar mixing applications. © 2013 American Institute of Chemical Engineers AIChE J, 00: 000–000, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14074" xmlns="http://purl.org/rss/1.0/"><title>Proactive Fault-Tolerant Model Predictive Control</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14074</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Proactive Fault-Tolerant Model Predictive Control</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Liangfeng Lao, Matthew Ellis, Panagiotis D. Christofides</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-13T14:42:31.261396-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14074</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14074</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14074</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Fault-tolerant control methods have been extensively researched over the last 10 years in the context of chemical process control applications, and provide a natural framework for integrating process monitoring and control aspects in a way that not only fault detection and isolation but also control system reconfiguration is achieved in the event of a process or actuator fault. But almost all the efforts are focused on the reactive fault-tolerant control. As another way for fault-tolerant control, proactive fault-tolerant control has been a popular topic in the communication systems and aerospace control systems communities for the last 10 years. At this point, no work has been done on proactive fault-tolerant control within the context of chemical process control. Motivated by this, a proactive fault-tolerant Lyapunov-based model predictive controller (LMPC) that can effectively deal with an incipient control actuator fault is proposed. This approach to proactive fault-tolerant control combines the unique stability and robustness properties of LMPC as well as explicitly accounting for incipient control actuator faults in the formulation of the MPC. Our theoretical results are applied to a chemical process example, and different scenaria were simulated to demonstrate that the proposed proactive fault-tolerant model predictive control method can achieve practical stability and efficiently deal with a control actuator fault. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 00: 000–000, 2013</p></div>
]]></content:encoded><description>
Fault-tolerant control methods have been extensively researched over the last 10 years in the context of chemical process control applications, and provide a natural framework for integrating process monitoring and control aspects in a way that not only fault detection and isolation but also control system reconfiguration is achieved in the event of a process or actuator fault. But almost all the efforts are focused on the reactive fault-tolerant control. As another way for fault-tolerant control, proactive fault-tolerant control has been a popular topic in the communication systems and aerospace control systems communities for the last 10 years. At this point, no work has been done on proactive fault-tolerant control within the context of chemical process control. Motivated by this, a proactive fault-tolerant Lyapunov-based model predictive controller (LMPC) that can effectively deal with an incipient control actuator fault is proposed. This approach to proactive fault-tolerant control combines the unique stability and robustness properties of LMPC as well as explicitly accounting for incipient control actuator faults in the formulation of the MPC. Our theoretical results are applied to a chemical process example, and different scenaria were simulated to demonstrate that the proposed proactive fault-tolerant model predictive control method can achieve practical stability and efficiently deal with a control actuator fault. © 2013 American Institute of Chemical Engineers AIChE J, 00: 000–000, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14067" xmlns="http://purl.org/rss/1.0/"><title>Nanometric Thin Skinned Dual-Layer Hollow Fiber Membranes for Dehydration of Isopropanol</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14067</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Nanometric Thin Skinned Dual-Layer Hollow Fiber Membranes for Dehydration of Isopropanol</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yu Pan Tang, Natalia Widjojo, Tai Shung Chung, Martin Weber, Christian Maletzko</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-13T09:57:13.807-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14067</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14067</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14067</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separations: Materials, Devices and 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A novel sulfonated polyphenylsulfone (sPPSU)/polyphenylsulfone (PPSU)-based dual-layer hollow fiber membrane with a nanometric thin skin layer has been designed for biofuel dehydration via pervaporation. The thickness of skin selective layer is in the range of 15–90 nm under different spinning conditions measured by positron annihilation spectroscopy (PAS) coupled with a mono-energetic positron beam. The effects of outer-layer dope properties, coagulation temperature, and dope flow rate during spinning were systematically investigated. By tuning these spinning parameters, a high performance sPPSU/PPSU-based dual-layer hollow fiber membrane with desirable morphology was successfully obtained. Particularly owing to its nanometric thin skin layer, a high flux of 3.47 kg/m<sup>2</sup>h with a separation factor of 156 was achieved for dehydration of an 85 wt % isopropanol aqueous solution at 50°C. After post thermal treatment at 150°C for 2 h, the separation factor was dramatically improved to 687 while flux dropped to 2.30 kg/m<sup>2</sup>h, which make it comparable to the inorganic membranes. In addition, excellent correlations were found among the results from field emission scanning electron microscopy, PAS spectra, and separation performance. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 00: 000–000, 2013</p></div>
]]></content:encoded><description>
A novel sulfonated polyphenylsulfone (sPPSU)/polyphenylsulfone (PPSU)-based dual-layer hollow fiber membrane with a nanometric thin skin layer has been designed for biofuel dehydration via pervaporation. The thickness of skin selective layer is in the range of 15–90 nm under different spinning conditions measured by positron annihilation spectroscopy (PAS) coupled with a mono-energetic positron beam. The effects of outer-layer dope properties, coagulation temperature, and dope flow rate during spinning were systematically investigated. By tuning these spinning parameters, a high performance sPPSU/PPSU-based dual-layer hollow fiber membrane with desirable morphology was successfully obtained. Particularly owing to its nanometric thin skin layer, a high flux of 3.47 kg/m2h with a separation factor of 156 was achieved for dehydration of an 85 wt % isopropanol aqueous solution at 50°C. After post thermal treatment at 150°C for 2 h, the separation factor was dramatically improved to 687 while flux dropped to 2.30 kg/m2h, which make it comparable to the inorganic membranes. In addition, excellent correlations were found among the results from field emission scanning electron microscopy, PAS spectra, and separation performance. © 2013 American Institute of Chemical Engineers AIChE J, 00: 000–000, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14033" xmlns="http://purl.org/rss/1.0/"><title>Selective Oxidation of Methanol to Dimethoxymethane over Mesoporous Al-P-V-O Catalysts</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14033</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Selective Oxidation of Methanol to Dimethoxymethane over Mesoporous Al-P-V-O Catalysts</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Shuang Chen, Yali Meng, Yujun Zhao, Xinbin Ma, Jinlong Gong</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-12T08:01:54.749762-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14033</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14033</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14033</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The synthesis and application of bifunctional mesoporous Al-P-V—O catalysts with both acidic and redox sites for selective oxidation of methanol to dimethoxymethane (DMM) is described. The catalysts were characterized by N<sub>2</sub> adsorption/desorption, X-ray diffraction, temperature-programmed desorption, X-ray photoelectron spectroscopy, and infrared spectroscopy. It is shown that porosity; redox property and surface acidity of the catalysts were greatly influenced by the Al/V/P ratio. The synergistic effect of phosphorus and vanadium was investigated. Al-P-V—O catalysts exhibited good catalytic activity because of the controlled reducibility and the acidic sites. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 00: 000–000, 2013</p></div>
]]></content:encoded><description>
The synthesis and application of bifunctional mesoporous Al-P-V—O catalysts with both acidic and redox sites for selective oxidation of methanol to dimethoxymethane (DMM) is described. The catalysts were characterized by N2 adsorption/desorption, X-ray diffraction, temperature-programmed desorption, X-ray photoelectron spectroscopy, and infrared spectroscopy. It is shown that porosity; redox property and surface acidity of the catalysts were greatly influenced by the Al/V/P ratio. The synergistic effect of phosphorus and vanadium was investigated. Al-P-V—O catalysts exhibited good catalytic activity because of the controlled reducibility and the acidic sites. © 2013 American Institute of Chemical Engineers AIChE J, 00: 000–000, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14060" xmlns="http://purl.org/rss/1.0/"><title>Thinnest Uniform Liquid Films Formed at the Highest Speeds with Reverse Roll Coating</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14060</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Thinnest Uniform Liquid Films Formed at the Highest Speeds with Reverse Roll Coating</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">H. Benkreira, Y. Shibata, K. Ito</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-11T21:27:31.116087-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14060</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14060</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14060</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena and Fluid Mechanics</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Reverse roll coating is probably the most widely used coating operation, much less investigated than its counterpart and inherently unstable forward roll coating. A new data to complement earlier work which was limited to large gaps and thus “thick” films is presented. The intention is to assess the feasibility of reverse roll coating to yield very thin films (&lt;10 μm) at high speeds (&gt;1 m/s) for application in the newer technologies, such as the production of solar cells and plastic electronics. The data obtained demonstrate this is possible but at the lowest permissible gap (25–50 μm) with low-viscosity fluids (∼7 mPa s). The study also developed a new understanding of how instabilities are controlled. It was seen that the size of the inertia forces generated by the applicator roller in relation to surface tension, as expressed by the Weber number and not the applicator Capillary number (viscous forces/surface tension) which is the critical parameter. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 00: 000–000, 2013</p></div>
]]></content:encoded><description>
Reverse roll coating is probably the most widely used coating operation, much less investigated than its counterpart and inherently unstable forward roll coating. A new data to complement earlier work which was limited to large gaps and thus “thick” films is presented. The intention is to assess the feasibility of reverse roll coating to yield very thin films (&lt;10 μm) at high speeds (&gt;1 m/s) for application in the newer technologies, such as the production of solar cells and plastic electronics. The data obtained demonstrate this is possible but at the lowest permissible gap (25–50 μm) with low-viscosity fluids (∼7 mPa s). The study also developed a new understanding of how instabilities are controlled. It was seen that the size of the inertia forces generated by the applicator roller in relation to surface tension, as expressed by the Weber number and not the applicator Capillary number (viscous forces/surface tension) which is the critical parameter. © 2013 American Institute of Chemical Engineers AIChE J, 00: 000–000, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14058" xmlns="http://purl.org/rss/1.0/"><title>Evaluating mixture adsorption models using molecular simulation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14058</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Evaluating mixture adsorption models using molecular simulation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Joseph A. Swisher, Li-Chiang Lin, Jihan Kim, Berend Smit</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-07T16:30:00.151677-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14058</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14058</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14058</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Thermodynamics and Molecular-Scale 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The design of adsorption-based separation processes using novel adsorbents requires reliable data for the adsorption of fluid mixtures on candidate adsorbents. Due to the difficulty of generating sufficient data across possible operating conditions, process designs generally rely on interpolation of pure-component data using a model, most commonly ideal adsorbed solution theory (IAST), and related theories. There are many cases where IAST fails to provide an adequate description of mixture adsorption, usually due to the fact that practical adsorbents do not have uniform surfaces. We have evaluated the use of a segregated version of IAST, where competition is assumed to occur at isolated adsorption sites. This simple modification can provide the correct description of adsorption across a large range of pressures using ideal isotherm models. We also demonstrate the importance of identifying multiple sites even for weakly adsorbing components to provide the correct behavior at high pressure. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The design of adsorption-based separation processes using novel adsorbents requires reliable data for the adsorption of fluid mixtures on candidate adsorbents. Due to the difficulty of generating sufficient data across possible operating conditions, process designs generally rely on interpolation of pure-component data using a model, most commonly ideal adsorbed solution theory (IAST), and related theories. There are many cases where IAST fails to provide an adequate description of mixture adsorption, usually due to the fact that practical adsorbents do not have uniform surfaces. We have evaluated the use of a segregated version of IAST, where competition is assumed to occur at isolated adsorption sites. This simple modification can provide the correct description of adsorption across a large range of pressures using ideal isotherm models. We also demonstrate the importance of identifying multiple sites even for weakly adsorbing components to provide the correct behavior at high pressure. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14029" xmlns="http://purl.org/rss/1.0/"><title>CFD simulations of turbulent fluid flow and dust dispersion in the 20 liter explosion vessel</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14029</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">CFD simulations of turbulent fluid flow and dust dispersion in the 20 liter explosion vessel</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A. Benedetto, P. Russo, R. Sanchirico, V. Sarli</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-06T11:14:42.941906-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14029</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14029</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14029</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A CFD model was developed with the aim at simulating the turbulent flow field induced by dust feeding and dispersion within the 20 L bomb, and the associated effects on the distribution of dust concentration. The model was validated considering a set of data (pressure time histories and root mean square velocity) available in the literature. The time sequences of velocity vector and kinetic energy maps have shown that multiple turbulent vortex structures are established within the sphere. These vortices generate dead volumes for the dust which is pushed toward the walls of the sphere. The obtained results are relevant to the practice of dust explosion testing and the interpretation of test results and, then, they should be taken as reference to improve the conditions for standard tests. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
A CFD model was developed with the aim at simulating the turbulent flow field induced by dust feeding and dispersion within the 20 L bomb, and the associated effects on the distribution of dust concentration. The model was validated considering a set of data (pressure time histories and root mean square velocity) available in the literature. The time sequences of velocity vector and kinetic energy maps have shown that multiple turbulent vortex structures are established within the sphere. These vortices generate dead volumes for the dust which is pushed toward the walls of the sphere. The obtained results are relevant to the practice of dust explosion testing and the interpretation of test results and, then, they should be taken as reference to improve the conditions for standard tests. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14052" xmlns="http://purl.org/rss/1.0/"><title>Rheological evolution and crystallization response of molten coal ash slag at high temperatures</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14052</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Rheological evolution and crystallization response of molten coal ash slag at high temperatures</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Wenjia Song, Lihua Tang, Zibin Zhu, Yoshihiko Ninomiya</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-05T11:12:50.730686-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14052</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14052</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14052</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Biomolecular Engineering, Bioengineering, Biochemicals, Biofuels, and Food</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Ash-related problems are often the main reason for entrained-flow gasifiers and boilers unscheduled shut downs. Thus, understanding the high-temperature physical properties of molten coal ash slag may enable an accurate description of the condition of ash deposition in the gasifier and boiler. The evolution of the time dependence of rheological behaviors, including the viscosity and yield stress of the molten coal ash slag containing 0–35.51 vol % crystals at decreasing temperatures (1400–1280°C) and within 1.05 × 10<sup>5</sup> s, were investigated. Non-Newtonian behaviors, including shear thinning, become obvious with an increasing crystal contents. The trends in the change of crystal nucleation rate in molten coal ash slag are similar with those of the growth rate. Finally, the experimental results and the crystal-size distribution method are used to develop a semiempirical parameterization that describes the complex non-Newtonian rheology of crystal-bearing molten coal ash slag. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Ash-related problems are often the main reason for entrained-flow gasifiers and boilers unscheduled shut downs. Thus, understanding the high-temperature physical properties of molten coal ash slag may enable an accurate description of the condition of ash deposition in the gasifier and boiler. The evolution of the time dependence of rheological behaviors, including the viscosity and yield stress of the molten coal ash slag containing 0–35.51 vol % crystals at decreasing temperatures (1400–1280°C) and within 1.05 × 105 s, were investigated. Non-Newtonian behaviors, including shear thinning, become obvious with an increasing crystal contents. The trends in the change of crystal nucleation rate in molten coal ash slag are similar with those of the growth rate. Finally, the experimental results and the crystal-size distribution method are used to develop a semiempirical parameterization that describes the complex non-Newtonian rheology of crystal-bearing molten coal ash slag. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14062" xmlns="http://purl.org/rss/1.0/"><title>Beyond classical theory: Predicting the free energy barrier of bubble nucleation in polymer foaming</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14062</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Beyond classical theory: Predicting the free energy barrier of bubble nucleation in polymer foaming</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Isamu Kusaka, Manish Talreja, David L. Tomasko</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-04T14:20:18.583915-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14062</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14062</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14062</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Thermodynamics and Molecular-Scale 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Based on the Gibbs-Tolman-Koenig formalism, we considered the Tolman correction to the free energy barrier of bubble nucleation in polymer-gas binary mixtures. For this class of systems, the correction may be estimated with a reasonable accuracy using experimentally accessible macroscopic thermodynamic quantities only. Although the Tolman correction is applicable only in the low supersaturation regime, a simple ansatz regarding the supersaturation dependence of the Tolman length can be made to extend the usefulness of this approach and to yield the free energy barrier that vanishes at the mean-field spinodal as demanded by thermodynamic considerations. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Based on the Gibbs-Tolman-Koenig formalism, we considered the Tolman correction to the free energy barrier of bubble nucleation in polymer-gas binary mixtures. For this class of systems, the correction may be estimated with a reasonable accuracy using experimentally accessible macroscopic thermodynamic quantities only. Although the Tolman correction is applicable only in the low supersaturation regime, a simple ansatz regarding the supersaturation dependence of the Tolman length can be made to extend the usefulness of this approach and to yield the free energy barrier that vanishes at the mean-field spinodal as demanded by thermodynamic considerations. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14020" xmlns="http://purl.org/rss/1.0/"><title>Predicting the Solubility of Solid Phenanthrene: A Combined Molecular Simulation and Group Contribution Approach</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14020</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Predicting the Solubility of Solid Phenanthrene: A Combined Molecular Simulation and Group Contribution Approach</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Andrew S. Paluch, Edward J. Maginn</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-04T14:07:37.910141-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14020</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14020</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14020</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Thermodynamics and Molecular-Scale 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A simple correction to the infinite dilution activity coefficient computed via molecular simulation for a nonelectrolyte solid solute in solution is proposed. The methodology adopts the concept that the activity coefficient may be fundamentally interpreted as a product of a residual and combinatorial term. The residual contribution is assumed to be insensitive to concentration, and the combinatorial term is modeled using the athermal Flory–Huggins theory. The proposed method uses only properties for the solute computed at infinite dilution to estimate solution-phase properties at finite concentrations. Properties of the pure solid solute are estimated using the group contribution method of Gani and coworkers, allowing for efficient blind solubility predictions to be made. The method is applied to predict the solubility of solid phenanthrene in 17 different solvents. For all cases, the combinatorial correction lowers the predicted solubility relative to the infinite dilution approximation, and in general, improves agreement with experiment. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
A simple correction to the infinite dilution activity coefficient computed via molecular simulation for a nonelectrolyte solid solute in solution is proposed. The methodology adopts the concept that the activity coefficient may be fundamentally interpreted as a product of a residual and combinatorial term. The residual contribution is assumed to be insensitive to concentration, and the combinatorial term is modeled using the athermal Flory–Huggins theory. The proposed method uses only properties for the solute computed at infinite dilution to estimate solution-phase properties at finite concentrations. Properties of the pure solid solute are estimated using the group contribution method of Gani and coworkers, allowing for efficient blind solubility predictions to be made. The method is applied to predict the solubility of solid phenanthrene in 17 different solvents. For all cases, the combinatorial correction lowers the predicted solubility relative to the infinite dilution approximation, and in general, improves agreement with experiment. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14044" xmlns="http://purl.org/rss/1.0/"><title>Optimization problem with normally distributed uncertain parameters</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14044</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Optimization problem with normally distributed uncertain parameters</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Gennady M. Ostrovsky, Nadir N. Ziyatdinov, Tatiana V. Lapteva</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-04T13:11:37.552923-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14044</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14044</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14044</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The issue of chemical process optimization when at the operation stage the design specification should be met with some probability and the control variables can be changed has been considered. A common approach for solving the broad class of optimization problems with normally distributed uncertain parameters were developed. This class includes the one-stage and two-stage optimization problems with chance constraints. This approach is based on approximate transformation of chance constraints into deterministic ones. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The issue of chemical process optimization when at the operation stage the design specification should be met with some probability and the control variables can be changed has been considered. A common approach for solving the broad class of optimization problems with normally distributed uncertain parameters were developed. This class includes the one-stage and two-stage optimization problems with chance constraints. This approach is based on approximate transformation of chance constraints into deterministic ones. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14039" xmlns="http://purl.org/rss/1.0/"><title>Modeling and control of protein crystal shape and size in batch crystallization</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14039</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Modeling and control of protein crystal shape and size in batch crystallization</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Joseph Sang-Il Kwon, Michael Nayhouse, Panagiotis D. Christofides, Gerassimos Orkoulas</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-04T11:08:48.879555-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14039</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14039</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14039</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Particle Technology and Fluidization</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>In this work, the modeling and control of a batch crystallization process used to produce tetragonal hen egg white lysozyme crystals are studied. Two processes are considered, crystal nucleation and growth. Crystal nucleation rates are obtained from previous experiments. The growth of each crystal progresses via kinetic Monte Carlo simulations comprising of adsorption, desorption, and migration on the (110) and (101) faces. The expressions of the rate equations are similar to Durbin and Feher. To control the nucleation and growth of the protein crystals and produce a crystal population with desired shape and size, a model predictive control (MPC) strategy is implemented. Specifically, the steady-state growth rates for the (110) and (101) faces are computed and their ratio is expressed in terms of the temperature and protein concentration via a nonlinear algebraic equation. The MPC method is shown to successfully regulate both the crystal size and shape distributions to different set-point values. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
In this work, the modeling and control of a batch crystallization process used to produce tetragonal hen egg white lysozyme crystals are studied. Two processes are considered, crystal nucleation and growth. Crystal nucleation rates are obtained from previous experiments. The growth of each crystal progresses via kinetic Monte Carlo simulations comprising of adsorption, desorption, and migration on the (110) and (101) faces. The expressions of the rate equations are similar to Durbin and Feher. To control the nucleation and growth of the protein crystals and produce a crystal population with desired shape and size, a model predictive control (MPC) strategy is implemented. Specifically, the steady-state growth rates for the (110) and (101) faces are computed and their ratio is expressed in terms of the temperature and protein concentration via a nonlinear algebraic equation. The MPC method is shown to successfully regulate both the crystal size and shape distributions to different set-point values. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14059" xmlns="http://purl.org/rss/1.0/"><title>Interaction analysis and geometric interconnection decoupling for networks of process systems</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14059</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Interaction analysis and geometric interconnection decoupling for networks of process systems</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Denny Hioe, Jie Bao, Nicolas Hudon</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-04T11:04:01.306563-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14059</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14059</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14059</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The effects of interactions between nonlinear subprocesses on the stabilizability of plantwide systems via the concept of dissipative systems are studied. Conditions for which controlled variables of each interconnected subprocess can be driven to and maintained at their desired values are established through the application of interconnection decoupling techniques. The resulting decoupling feedback law encodes the interaction effects between subprocesses and determines the required information structure for achieving desired control performance using distributed control laws. The proposed constructive approach leads to new criteria for the selection of manipulated and controlled variables that guarantee plantwide stability. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The effects of interactions between nonlinear subprocesses on the stabilizability of plantwide systems via the concept of dissipative systems are studied. Conditions for which controlled variables of each interconnected subprocess can be driven to and maintained at their desired values are established through the application of interconnection decoupling techniques. The resulting decoupling feedback law encodes the interaction effects between subprocesses and determines the required information structure for achieving desired control performance using distributed control laws. The proposed constructive approach leads to new criteria for the selection of manipulated and controlled variables that guarantee plantwide stability. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14057" xmlns="http://purl.org/rss/1.0/"><title>Theoretical modeling coupled with experimental study on the preparation and characterization comparison of fluorinated copolymers: Effect of chain structure on copolymer properties</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14057</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Theoretical modeling coupled with experimental study on the preparation and characterization comparison of fluorinated copolymers: Effect of chain structure on copolymer properties</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yin-Ning Zhou, Zheng-Hong Luo, Jian-Hua Chen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-04T09:53:32.27793-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14057</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14057</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14057</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Soft Matter: Synthesis, Processing and Products</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Theoretical modeling coupled with an experimental study is presented for the preparation and characterization comparison of the amphiphilic copolymers of 2, 2, 3, 3, 4, 4, 4-heptafluorobutyl methacrylate (HFBMA) and 2-hydroxyethyl methacrylate (HEMA) to achieve a multiscale generalization of the polymeric system. A series of amphiphilic copolymers having different chain structures with HFBMA as the hydrophobic component and HEMA as the hydrophilic component was first synthesized through atom transfer radical copolymerization (ATRcoP) or model-based semibatch ATRcoP. Theoretical modeling is used to optimize the macromolecular structure and experimental approaches that are used to prepare copolymers of HFBMA and HEMA with some tailor-made polymer properties. Furthermore, a systematic comparison of major properties (i.e., thermal, micellization, and surface properties) of these fluorinated copolymers (i.e., random, block, linear gradient, and inverse linear gradient copolymers) was carried out. The results show that these fluorinated copolymers with different chain structures have dissimilar properties. The results also demonstrate that the approach of coupling theoretical modeling with an experimental study can be used to guide a multiscale generalization of the polymeric system for practical application. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Theoretical modeling coupled with an experimental study is presented for the preparation and characterization comparison of the amphiphilic copolymers of 2, 2, 3, 3, 4, 4, 4-heptafluorobutyl methacrylate (HFBMA) and 2-hydroxyethyl methacrylate (HEMA) to achieve a multiscale generalization of the polymeric system. A series of amphiphilic copolymers having different chain structures with HFBMA as the hydrophobic component and HEMA as the hydrophilic component was first synthesized through atom transfer radical copolymerization (ATRcoP) or model-based semibatch ATRcoP. Theoretical modeling is used to optimize the macromolecular structure and experimental approaches that are used to prepare copolymers of HFBMA and HEMA with some tailor-made polymer properties. Furthermore, a systematic comparison of major properties (i.e., thermal, micellization, and surface properties) of these fluorinated copolymers (i.e., random, block, linear gradient, and inverse linear gradient copolymers) was carried out. The results show that these fluorinated copolymers with different chain structures have dissimilar properties. The results also demonstrate that the approach of coupling theoretical modeling with an experimental study can be used to guide a multiscale generalization of the polymeric system for practical application. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14042" xmlns="http://purl.org/rss/1.0/"><title>Simulations of vapor–liquid phase equilibrium and interfacial tension in the CO2–H2O–NaCl system</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14042</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Simulations of vapor–liquid phase equilibrium and interfacial tension in the CO2–H2O–NaCl system</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yang Liu, Thomas Lafitte, Athanassios Z. Panagiotopoulos, Pablo G. Debenedetti</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-01T18:03:34.396845-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14042</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14042</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14042</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. Thermodynamics and Molecular-Scale 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Direct interfacial molecular dynamics simulations are used to obtain the phase behavior and interfacial tension of CO<sub>2</sub>–H<sub>2</sub>O–NaCl mixtures over a broad temperature and pressure range (50°C ≤ T ≤ 250°C, 0 ≤ P ≤ 600 bar) and NaCl concentrations (1–4 mol/kg H<sub>2</sub>O). The predictive ability of several existing water (SPC and TIP4P2005), carbon dioxide (EPM2 and TraPPE), and sodium chloride (SD and DRVH) models is studied and compared, using conventional Lorentz–Berthelot combining rules for the unlike-pair parameters. Under conditions of moderate NaCl molality (∼1 mol/kg H<sub>2</sub>O), the predictions of the CO<sub>2</sub> solubility in the water-rich and CO<sub>2</sub>-rich phase resemble those in the CO<sub>2</sub>–H<sub>2</sub>O system [Liu et al., J Phys Chem B. 2011;115:6629–6635]. Consistent with our previous work, the TraPPE/TIP4P2005 model combination gives the best overall performance in predicting coexistence composition and pressure in the water-rich phase. Critical assessments are also made on the ranges of temperature and pressure where particular model combinations work better. The dependence of the interfacial tension on temperature and pressure is better predicted by the TraPPE/TIP4P2005 and EPM2/SPC models, whereas the EPM2/TIP4P2005 model overestimates this property by 10–20%, possibly due to the inadequacy of the combining rules. It is also found that the interfacial tension increases with salt concentration, consistent with experimental observations. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Direct interfacial molecular dynamics simulations are used to obtain the phase behavior and interfacial tension of CO2–H2O–NaCl mixtures over a broad temperature and pressure range (50°C ≤ T ≤ 250°C, 0 ≤ P ≤ 600 bar) and NaCl concentrations (1–4 mol/kg H2O). The predictive ability of several existing water (SPC and TIP4P2005), carbon dioxide (EPM2 and TraPPE), and sodium chloride (SD and DRVH) models is studied and compared, using conventional Lorentz–Berthelot combining rules for the unlike-pair parameters. Under conditions of moderate NaCl molality (∼1 mol/kg H2O), the predictions of the CO2 solubility in the water-rich and CO2-rich phase resemble those in the CO2–H2O system [Liu et al., J Phys Chem B. 2011;115:6629–6635]. Consistent with our previous work, the TraPPE/TIP4P2005 model combination gives the best overall performance in predicting coexistence composition and pressure in the water-rich phase. Critical assessments are also made on the ranges of temperature and pressure where particular model combinations work better. The dependence of the interfacial tension on temperature and pressure is better predicted by the TraPPE/TIP4P2005 and EPM2/SPC models, whereas the EPM2/TIP4P2005 model overestimates this property by 10–20%, possibly due to the inadequacy of the combining rules. It is also found that the interfacial tension increases with salt concentration, consistent with experimental observations. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14053" xmlns="http://purl.org/rss/1.0/"><title>Particle-in-cell simulation of electron and ion energy distributions in dc/rf hybrid capacitively-coupled plasmas</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14053</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Particle-in-cell simulation of electron and ion energy distributions in dc/rf hybrid capacitively-coupled plasmas</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Paola Diomede, Doosik Kim, Demetre J. Economou</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-01T17:19:18.624158-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14053</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14053</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14053</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. Inorganic Materials: Synthesis and Processing</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A Particle-in-Cell simulation with Monte Carlo collisions was used to study electron and ion energy distributions (IEDs) in low-pressure (2.67 Pa) direct-current (dc)/radio-frequency (rf) hybrid capacitively-coupled Ar plasmas. One electrode (dc/rf electrode) of the parallel plate diode was powered by a 13.56 MHz source, and a negative dc bias voltage, whereas the opposite (substrate) electrode was grounded. Secondary electrons emitted from the dc/rf electrode accelerated in the adjacent sheath and entered the plasma, yielding a high-energy tail of the electron energy distribution. For given dc bias voltage, the plasma density increased as the secondary electron emission yield due to ion bombardment increased. A fraction of the secondary electrons were energetic enough to overcome the sheath potential barrier on the substrate electrode and bombard the substrate. The electron angular distribution on the substrate electrode had a peak of directional electrons superimposed on a typical cosine distribution. The mean energy and angular spread of directional electrons could be controlled by varying the dc bias voltage. However, as the dc bias became more negative, the dc/rf sheath expanded at the expense of the bulk plasma, reducing the plasma density, in agreement with published data. The IED on the substrate electrode exhibited a dominant bimodal feature with multiple shoulder peaks due to ion-neutral charge exchange collisions. The average ion energy decreased as the dc voltage became more negative, also in agreement with data. Pulsing the plasma power enhanced the tail of the electron energy distribution in the early activeglow (power ON), and yielded a distinct ballistic electron flux on the substrate with energy equal to the applied dc bias. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
A Particle-in-Cell simulation with Monte Carlo collisions was used to study electron and ion energy distributions (IEDs) in low-pressure (2.67 Pa) direct-current (dc)/radio-frequency (rf) hybrid capacitively-coupled Ar plasmas. One electrode (dc/rf electrode) of the parallel plate diode was powered by a 13.56 MHz source, and a negative dc bias voltage, whereas the opposite (substrate) electrode was grounded. Secondary electrons emitted from the dc/rf electrode accelerated in the adjacent sheath and entered the plasma, yielding a high-energy tail of the electron energy distribution. For given dc bias voltage, the plasma density increased as the secondary electron emission yield due to ion bombardment increased. A fraction of the secondary electrons were energetic enough to overcome the sheath potential barrier on the substrate electrode and bombard the substrate. The electron angular distribution on the substrate electrode had a peak of directional electrons superimposed on a typical cosine distribution. The mean energy and angular spread of directional electrons could be controlled by varying the dc bias voltage. However, as the dc bias became more negative, the dc/rf sheath expanded at the expense of the bulk plasma, reducing the plasma density, in agreement with published data. The IED on the substrate electrode exhibited a dominant bimodal feature with multiple shoulder peaks due to ion-neutral charge exchange collisions. The average ion energy decreased as the dc voltage became more negative, also in agreement with data. Pulsing the plasma power enhanced the tail of the electron energy distribution in the early activeglow (power ON), and yielded a distinct ballistic electron flux on the substrate with energy equal to the applied dc bias. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14046" xmlns="http://purl.org/rss/1.0/"><title>Computational screening of porous carbons, zeolites, and metal organic frameworks for desulfurization and decarburization of biogas, natural gas, and flue gas</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14046</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Computational screening of porous carbons, zeolites, and metal organic frameworks for desulfurization and decarburization of biogas, natural gas, and flue gas</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Xuan Peng, Dapeng Cao</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-27T17:49:31.072813-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14046</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14046</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14046</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separations: Materials, Devices and 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Eighteen kinds of porous materials from carbons, zeolites, and metal organic frameworks (MOFs) have been extensively investigated for desulfurization and decarburization of the biogas, natural gas, and flue gas by using a molecular modeling approach. By considering not only the selectivity but also capacity, Na-5A, zeolite-like MOF (zMOF), and Na-13X, MIL-47 are screened as the most promising candidates for removal of sulfide in the CH<sub>4</sub><img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>CO<sub>2</sub><img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>H<sub>2</sub>S and N<sub>2</sub><img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>CO<sub>2</sub><img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>SO<sub>2</sub> systems, respectively. However, for simultaneous removal of sulfide and CO<sub>2</sub>, the best candidates are zMOF for the natural gas and biogas (i.e., CH<sub>4</sub><img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>CO<sub>2</sub><img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>H<sub>2</sub>S system) and MOF-74-Zn for the flue gas (i.e., N<sub>2</sub><img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>CO<sub>2</sub><img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>SO<sub>2</sub> system). Moreover, the regeneration ability of the recommended adsorbents is further assessed by studying the effect of temperature on adsorption. It is found that compared to the zMOF and MIL-47 MOFs, the Na-5A and Na-13X zeolites are not easily regenerated due to the difficulty in desorption of sulfide at high temperature, which results from the stronger adsorbent–adsorbate interactions in zeolites. The effect of sulfide concentration on the adsorption properties of the recommended adsorbents is also explored. We observe that the zMOF and MIL-47 are also superior to the Na-5A and Na-13X for desulfurization of gas mixtures containing high sulfide concentration. This is because MOFs with larger pore volume lead to a greater sulfide uptake. The effects of porosity, framework density, pore volume, and accessible surface area on the separation performance are analyzed. The optimum porosity is about 0.5–0.6, to meet the requirements of both high selectivity and uptake. It is expected this work provides a useful guidance for the practical applications of desulfurization and decarburization. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Eighteen kinds of porous materials from carbons, zeolites, and metal organic frameworks (MOFs) have been extensively investigated for desulfurization and decarburization of the biogas, natural gas, and flue gas by using a molecular modeling approach. By considering not only the selectivity but also capacity, Na-5A, zeolite-like MOF (zMOF), and Na-13X, MIL-47 are screened as the most promising candidates for removal of sulfide in the CH4<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>CO2<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>H2S and N2<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>CO2<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>SO2 systems, respectively. However, for simultaneous removal of sulfide and CO2, the best candidates are zMOF for the natural gas and biogas (i.e., CH4<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>CO2<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>H2S system) and MOF-74-Zn for the flue gas (i.e., N2<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>CO2<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>SO2 system). Moreover, the regeneration ability of the recommended adsorbents is further assessed by studying the effect of temperature on adsorption. It is found that compared to the zMOF and MIL-47 MOFs, the Na-5A and Na-13X zeolites are not easily regenerated due to the difficulty in desorption of sulfide at high temperature, which results from the stronger adsorbent–adsorbate interactions in zeolites. The effect of sulfide concentration on the adsorption properties of the recommended adsorbents is also explored. We observe that the zMOF and MIL-47 are also superior to the Na-5A and Na-13X for desulfurization of gas mixtures containing high sulfide concentration. This is because MOFs with larger pore volume lead to a greater sulfide uptake. The effects of porosity, framework density, pore volume, and accessible surface area on the separation performance are analyzed. The optimum porosity is about 0.5–0.6, to meet the requirements of both high selectivity and uptake. It is expected this work provides a useful guidance for the practical applications of desulfurization and decarburization. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14025" xmlns="http://purl.org/rss/1.0/"><title>Prediction of particle charging in a dilute pneumatic conveying system</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14025</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Prediction of particle charging in a dilute pneumatic conveying system</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Poom Bunchatheeravate, Jennifer Curtis, Yusuke Fujii, Shuji Matsusaka</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-27T17:25:52.727307-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14025</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14025</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14025</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Particle Technology and Fluidization</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>When particles are transported in pipelines, they acquire electrostatic charges as they come into contact with the pipe wall. Charged particles can cause problems such as particle agglomeration, blockage, and explosion. Understanding the particle charge can help to prevent these issues. This study investigates a technique for predicting the particle charge in a straight pipe of any given length, as well as the pipe length at which electrostatic equilibrium occurs, through experimentation in a short 1-m pipe section. Experimentation with five different types of particles and four pipe wall materials at longer pipe lengths were used to validate the technique. This predictive technique is applicable to a range of particle shapes and sizes under the restriction that charge transfer is due to impact charging. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
When particles are transported in pipelines, they acquire electrostatic charges as they come into contact with the pipe wall. Charged particles can cause problems such as particle agglomeration, blockage, and explosion. Understanding the particle charge can help to prevent these issues. This study investigates a technique for predicting the particle charge in a straight pipe of any given length, as well as the pipe length at which electrostatic equilibrium occurs, through experimentation in a short 1-m pipe section. Experimentation with five different types of particles and four pipe wall materials at longer pipe lengths were used to validate the technique. This predictive technique is applicable to a range of particle shapes and sizes under the restriction that charge transfer is due to impact charging. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14050" xmlns="http://purl.org/rss/1.0/"><title>What controls dynamics of droplet shape evolution upon impingement on a solid surface?</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14050</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">What controls dynamics of droplet shape evolution upon impingement on a solid surface?</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Wenchao Zhou, Drew Loney, F. Levent Degertekin, David W. Rosen, Andrei G. Fedorov</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-27T16:39:59.163254-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14050</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14050</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14050</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena and Fluid Mechanics</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A shape coefficient is introduced to quantify droplet shape by measuring its similarity to a desired shape to enable the study of droplet shape evolution upon impingement on a solid surface. Parametric simulations are performed with an experimentally validated numerical model to determine the impact conditions to maximize the shape coefficient. Results show that the Weber number is the controlling factor that determines the maximum achievable shape coefficient and the time instant when it is achieved for small Ohnesorge numbers, whereas the Reynolds number becomes the key parameter defining the optimal shape when the Ohnesorge number is large. A regime map is also developed to define the regions where a desired droplet shape can be achieved without splash. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
A shape coefficient is introduced to quantify droplet shape by measuring its similarity to a desired shape to enable the study of droplet shape evolution upon impingement on a solid surface. Parametric simulations are performed with an experimentally validated numerical model to determine the impact conditions to maximize the shape coefficient. Results show that the Weber number is the controlling factor that determines the maximum achievable shape coefficient and the time instant when it is achieved for small Ohnesorge numbers, whereas the Reynolds number becomes the key parameter defining the optimal shape when the Ohnesorge number is large. A regime map is also developed to define the regions where a desired droplet shape can be achieved without splash. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14054" xmlns="http://purl.org/rss/1.0/"><title>Integrated combined cycle from natural gas with CO2 capture using a Ca–Cu chemical loop</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14054</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Integrated combined cycle from natural gas with CO2 capture using a Ca–Cu chemical loop</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Isabel Martínez, Ramon Murillo, Gemma Grasa, Jose R. Fernández, Juan Carlos Abanades</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-27T16:27:00.048019-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14054</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14054</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14054</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The integration in a natural gas combined cycle (NGCC) of a novel process for H<sub>2</sub> production using a chemical Ca–Cu loop was proposed. This process is based on the sorption-enhanced reforming process for H<sub>2</sub> production from natural gas with a CaO/CaCO<sub>3</sub> chemical loop, but including a second Cu/CuO loop to regenerate the Ca-sorbent. An integration of this system into a NGCC was proposed and a full process simulation exercise of different cases was carried out. Optimizing the operating conditions in the Ca–Cu looping process, 8.1% points of efficiency penalty with respect to a state-of-the-art NGCC are obtained with a CO<sub>2</sub> capture efficiency of 90%. It was demonstrated that the new process can yield power generation efficiencies as high as any other emerging and commercial concepts for power generation from NGCC with CO<sub>2</sub> capture, but maintaining competing advantages of process simplification and compact pressurized reactor design inherent to the Ca–Cu looping system. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The integration in a natural gas combined cycle (NGCC) of a novel process for H2 production using a chemical Ca–Cu loop was proposed. This process is based on the sorption-enhanced reforming process for H2 production from natural gas with a CaO/CaCO3 chemical loop, but including a second Cu/CuO loop to regenerate the Ca-sorbent. An integration of this system into a NGCC was proposed and a full process simulation exercise of different cases was carried out. Optimizing the operating conditions in the Ca–Cu looping process, 8.1% points of efficiency penalty with respect to a state-of-the-art NGCC are obtained with a CO2 capture efficiency of 90%. It was demonstrated that the new process can yield power generation efficiencies as high as any other emerging and commercial concepts for power generation from NGCC with CO2 capture, but maintaining competing advantages of process simplification and compact pressurized reactor design inherent to the Ca–Cu looping system. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14051" xmlns="http://purl.org/rss/1.0/"><title>Multiway independent component analysis mixture model and mutual information based fault detection and diagnosis approach of multiphase batch processes</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14051</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Multiway independent component analysis mixture model and mutual information based fault detection and diagnosis approach of multiphase batch processes</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jie Yu, Jingyan Chen, Mudassir M. Rashid</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-27T16:03:48.61036-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14051</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14051</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14051</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Batch process monitoring is a challenging task, because conventional methods are not well suited to handle the inherent multiphase operation. In this study, a novel multiway independent component analysis (MICA) mixture model and mutual information based fault detection and diagnosis approach is proposed. The multiple operating phases in batch processes are characterized by non-Gaussian independent component mixture models. Then, the posterior probability of the monitored sample is maximized to identify the operating phase that the sample belongs to, and, thus, the localized MICA model is developed for process fault detection. Moreover, the detected faulty samples are projected onto the residual subspace, and the mutual information based non-Gaussian contribution index is established to evaluate the statistical dependency between the projection and the measurement along each process variable. Such contribution index is used to diagnose the major faulty variables responsible for process abnormalities. The effectiveness of the proposed approach is demonstrated using the fed-batch penicillin fermentation process, and the results are compared to those of the multiway principal component analysis mixture model and regular MICA method. The case study demonstrates that the proposed approach is able to detect the abnormal events over different phases as well as diagnose the faulty variables with high accuracy. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Batch process monitoring is a challenging task, because conventional methods are not well suited to handle the inherent multiphase operation. In this study, a novel multiway independent component analysis (MICA) mixture model and mutual information based fault detection and diagnosis approach is proposed. The multiple operating phases in batch processes are characterized by non-Gaussian independent component mixture models. Then, the posterior probability of the monitored sample is maximized to identify the operating phase that the sample belongs to, and, thus, the localized MICA model is developed for process fault detection. Moreover, the detected faulty samples are projected onto the residual subspace, and the mutual information based non-Gaussian contribution index is established to evaluate the statistical dependency between the projection and the measurement along each process variable. Such contribution index is used to diagnose the major faulty variables responsible for process abnormalities. The effectiveness of the proposed approach is demonstrated using the fed-batch penicillin fermentation process, and the results are compared to those of the multiway principal component analysis mixture model and regular MICA method. The case study demonstrates that the proposed approach is able to detect the abnormal events over different phases as well as diagnose the faulty variables with high accuracy. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14007" xmlns="http://purl.org/rss/1.0/"><title>Effect of boric acid on thermal dehydrogenation of ammonia borane: H2 yield and process characteristics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14007</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effect of boric acid on thermal dehydrogenation of ammonia borane: H2 yield and process characteristics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hyun Tae Hwang, Patrick Greenan, Seung Jin Kim, Arvind Varma</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-27T13:52:06.425012-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14007</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14007</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14007</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. Reaction Engineering, 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>We have recently demonstrated that boric acid (H<sub>3</sub>BO<sub>3</sub>, BA) is a promising additive to decrease onset temperature as well as to enhance hydrogen release kinetics for thermolysis of ammonia borane (NH<sub>3</sub>BH<sub>3</sub>, AB). The observations suggest that tetrahydroxyborate ion released by heating BA serves as Lewis acid and catalyzes AB dehydrogenation. Using this approach, we obtained high H<sub>2</sub> yield at 85°C, along with rapid kinetics. Various operating conditions were investigated, such as reactor temperature, AB wt %, and particle size of BA. Even in the presence of 10 wt % BA, high H<sub>2</sub> yield (13 wt %) and trace amount of ammonia (10–20 ppm) were obtained at 80°C, proton exchange membrane (PEM) fuel cell operating temperature. To our knowledge, such H<sub>2</sub> yield value is higher than from any other method using AB with additive or catalyst at PEM fuel cell operating temperatures. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
We have recently demonstrated that boric acid (H3BO3, BA) is a promising additive to decrease onset temperature as well as to enhance hydrogen release kinetics for thermolysis of ammonia borane (NH3BH3, AB). The observations suggest that tetrahydroxyborate ion released by heating BA serves as Lewis acid and catalyzes AB dehydrogenation. Using this approach, we obtained high H2 yield at 85°C, along with rapid kinetics. Various operating conditions were investigated, such as reactor temperature, AB wt %, and particle size of BA. Even in the presence of 10 wt % BA, high H2 yield (13 wt %) and trace amount of ammonia (10–20 ppm) were obtained at 80°C, proton exchange membrane (PEM) fuel cell operating temperature. To our knowledge, such H2 yield value is higher than from any other method using AB with additive or catalyst at PEM fuel cell operating temperatures. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14012" xmlns="http://purl.org/rss/1.0/"><title>Optimal Design of Generalized Batch-Storage Network Considering Shortage Costs</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14012</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Optimal Design of Generalized Batch-Storage Network Considering Shortage Costs</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Gyeongbeom Yi, Gintaras V. Reklaitis</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-27T13:21:18.373362-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14012</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14012</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14012</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Product shortages, which cause backlogging and/or lost sales costs commonly occur in the chemical industries, especially in the commodity polymer business. Shortage costs in a supply chain optimization model are studied under the framework of a generalized batch-storage network. A classical economic order quantity model with backlogging costs suggested an optimal time delay and final product delivery lot size. A product shortage can be mitigated by advancing production/transportation or by purchasing a substitute product from a third party as well as by a product delivery delay in the supply chain network. Optimal solutions that consider all means for recovering shortage are more complicated than the classical case. Four solutions are identified depending on the parametric range and variable bounds. The optimal capacity for production/transportation processes associated with a product in shortage can differ from that of a product not in shortage. An illustrative example is presented in support of the analytical results. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Product shortages, which cause backlogging and/or lost sales costs commonly occur in the chemical industries, especially in the commodity polymer business. Shortage costs in a supply chain optimization model are studied under the framework of a generalized batch-storage network. A classical economic order quantity model with backlogging costs suggested an optimal time delay and final product delivery lot size. A product shortage can be mitigated by advancing production/transportation or by purchasing a substitute product from a third party as well as by a product delivery delay in the supply chain network. Optimal solutions that consider all means for recovering shortage are more complicated than the classical case. Four solutions are identified depending on the parametric range and variable bounds. The optimal capacity for production/transportation processes associated with a product in shortage can differ from that of a product not in shortage. An illustrative example is presented in support of the analytical results. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14047" xmlns="http://purl.org/rss/1.0/"><title>Ionic liquids: Solubility parameters and selectivities for organic solutes</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14047</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Ionic liquids: Solubility parameters and selectivities for organic solutes</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Li-Sheng Wang, Xin-Xin Wang, Yi Li, Kan Jiang, Xian-Zhao Shao, Chao-Jun Du</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-26T12:25:29.50863-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14047</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14047</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14047</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Thermodynamics and Molecular-Scale 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Ionic liquids (ILs) are innovative solvents for chemical processing. In this work, a database on activity coefficients of organic solutes at infinite dilution in ILs was collected from literature sources. The activity coefficients have been correlated by activity coefficient model for the regular solution and have been used to estimate the solubility parameter of ILs. The solubility parameters of ILs have been further correlated based on a concept of the group contribution method. Through the analysis of the database and the prediction results of selectivities, it was shown here that as compared with conventional organic solvents, higher selectivity can be achieved by using ILs as working solvents for separation of alkane/aromatic, aromatic/aromatic hydrocarbon mixtures via extraction or supported liquid membrane. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Ionic liquids (ILs) are innovative solvents for chemical processing. In this work, a database on activity coefficients of organic solutes at infinite dilution in ILs was collected from literature sources. The activity coefficients have been correlated by activity coefficient model for the regular solution and have been used to estimate the solubility parameter of ILs. The solubility parameters of ILs have been further correlated based on a concept of the group contribution method. Through the analysis of the database and the prediction results of selectivities, it was shown here that as compared with conventional organic solvents, higher selectivity can be achieved by using ILs as working solvents for separation of alkane/aromatic, aromatic/aromatic hydrocarbon mixtures via extraction or supported liquid membrane. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14000" xmlns="http://purl.org/rss/1.0/"><title>Active fault isolation of nonlinear process systems</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14000</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Active fault isolation of nonlinear process systems</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Miao Du, Prashant Mhaskar</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T18:00:54.347993-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14000</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14000</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14000</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>This work considers the problem of designing an active fault-isolation scheme for nonlinear process systems subject to uncertainty. The faults under consideration include bounded actuator faults and process disturbances. The key idea of the proposed method is to exploit the nonlinear way that faults affect the process evolution through supervisory feedback control. To this end, a dedicated fault-isolation residual and its time-varying threshold are generated for each fault by treating other faults as disturbances. A fault is isolated when the corresponding residual breaches its threshold. These residuals, however, may not be sensitive to faults in the operating region under nominal operation. To make these residuals sensitive to faults, a switching rule is designed to drive the process states, upon detection of a fault, to move toward an operating point that, for any given fault, results in the reduction of the effect of other faults on the evolution of the same process state. This idea is then generalized to sequentially operate the process at multiple operating points that facilitate isolation of different faults for the case where the residuals are not simultaneously sensitive to faults at a single operating point. The effectiveness of the proposed active fault-isolation scheme is illustrated using a chemical reactor example and demonstrated through application to a solution copolymerization of methyl methacrylate and vinyl acetate. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
This work considers the problem of designing an active fault-isolation scheme for nonlinear process systems subject to uncertainty. The faults under consideration include bounded actuator faults and process disturbances. The key idea of the proposed method is to exploit the nonlinear way that faults affect the process evolution through supervisory feedback control. To this end, a dedicated fault-isolation residual and its time-varying threshold are generated for each fault by treating other faults as disturbances. A fault is isolated when the corresponding residual breaches its threshold. These residuals, however, may not be sensitive to faults in the operating region under nominal operation. To make these residuals sensitive to faults, a switching rule is designed to drive the process states, upon detection of a fault, to move toward an operating point that, for any given fault, results in the reduction of the effect of other faults on the evolution of the same process state. This idea is then generalized to sequentially operate the process at multiple operating points that facilitate isolation of different faults for the case where the residuals are not simultaneously sensitive to faults at a single operating point. The effectiveness of the proposed active fault-isolation scheme is illustrated using a chemical reactor example and demonstrated through application to a solution copolymerization of methyl methacrylate and vinyl acetate. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14027" xmlns="http://purl.org/rss/1.0/"><title>A new dry tray pressure drop model of float valve trays</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14027</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A new dry tray pressure drop model of float valve trays</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jun Wang, Yi-Xuan Tang, Yan-Sheng Liu, Rui Cao, Tian-Xin Chen, Yu-Feng Hu, Xue-Jun Fan</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T17:41:58.534952-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14027</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14027</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14027</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena and Fluid Mechanics</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>An accurate prediction of the dry pressure drop is very important for consideration of valve trays and for calculations in distillation field. Therefore, in this article, a series of hydraulic experiments were first conducted to reveal that the intermediate state during the valve opening process is closely related to the dry tray pressure drop under great valve weight. Then, a rigorous force analysis was made to show that Euler number is related only to the valve's position at the balance points for a certain valve type. Third, a new model for prediction of the dry tray pressure drop—which considers for the first time the influence of the intermediate state—was developed and then simplified for the purpose of convenient utilizations. Finally, the new model and its simplified form were tested by comparisons with the experimental results. The agreements are good, with the mean deviations being &lt;5%. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
An accurate prediction of the dry pressure drop is very important for consideration of valve trays and for calculations in distillation field. Therefore, in this article, a series of hydraulic experiments were first conducted to reveal that the intermediate state during the valve opening process is closely related to the dry tray pressure drop under great valve weight. Then, a rigorous force analysis was made to show that Euler number is related only to the valve's position at the balance points for a certain valve type. Third, a new model for prediction of the dry tray pressure drop—which considers for the first time the influence of the intermediate state—was developed and then simplified for the purpose of convenient utilizations. Finally, the new model and its simplified form were tested by comparisons with the experimental results. The agreements are good, with the mean deviations being &lt;5%. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14037" xmlns="http://purl.org/rss/1.0/"><title>Probability distributions of gas hydrate formation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14037</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Probability distributions of gas hydrate formation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Reuben Wu, Karen A. Kozielski, Patrick G. Hartley, Eric F. May, John Boxall, Nobuo Maeda</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T16:21:56.549996-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14037</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14037</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14037</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Thermodynamics and Molecular-Scale 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Induction time distributions for gas hydrate formation were measured for gas mixtures of methane + propane at pressures up to 11.3 MPa using a high-pressure automated lag time apparatus (HP-ALTA). Measurements were made at subcooling temperatures between 4.3 and 13.5 K and, while isothermal induction times between 0 and 15,000 s were observed, the median isothermal induction times for the distributions ranged from 100 to 4000 s. A hyperbolic relationship between median induction time and subcooling was used to correlate the data. A graphical interpretation is presented that relates the two types of data that can be acquired by using the HP-ALTA in one of two modes to study hydrate formation: induction time distributions at constant subcooling and formation temperature distributions observed during linear cooling ramps. The equivalence of these two modes provides a robust method for studying the variation of formation phenomena in different hydrate systems. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Induction time distributions for gas hydrate formation were measured for gas mixtures of methane + propane at pressures up to 11.3 MPa using a high-pressure automated lag time apparatus (HP-ALTA). Measurements were made at subcooling temperatures between 4.3 and 13.5 K and, while isothermal induction times between 0 and 15,000 s were observed, the median isothermal induction times for the distributions ranged from 100 to 4000 s. A hyperbolic relationship between median induction time and subcooling was used to correlate the data. A graphical interpretation is presented that relates the two types of data that can be acquired by using the HP-ALTA in one of two modes to study hydrate formation: induction time distributions at constant subcooling and formation temperature distributions observed during linear cooling ramps. The equivalence of these two modes provides a robust method for studying the variation of formation phenomena in different hydrate systems. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14041" xmlns="http://purl.org/rss/1.0/"><title>PDA measurements in a three-phase bubble column</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14041</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">PDA measurements in a three-phase bubble column</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Z. W. Gan, S. C. M. Yu, A. W. K. Law</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T16:10:46.102453-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14041</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14041</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14041</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Biomolecular Engineering, Bioengineering, Biochemicals, Biofuels, and Food</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Phase Doppler anemometry was used to quantify the flow characteristic of a three phases (liquid, solid, and bubbles) cylindrical bubble column driven by a point air source made of a 30-mm diameter perforated air stone centrally mounted at the bottom. The cylindrical bubble column had an inner diameter of 152 mm and was filled with liquid up to 1 m above the point source. Acrylic beads with a nominal diameter of 3 mm were used as the solid phase. To match the density of the solid phase which was 1.05 kg/m<sup>3</sup>, the liquid density was raised to about 1.0485 kg/m3 by added salt. The bubble diameters generated were within the range of 600–2400 µm. The detailed turbulent characteristics of the liquid-phase velocity, bubble diameter, bubble velocity, and solid velocity were measured at three different air rates, namely 0.4, 0.8, and 1.2 L/min (corresponding to average gas volume fraction of 0.0084, 0.0168, and 0.0258, respectively) for the homogeneous bubble column regime. With the addition of the solid phase, the flow field was found to be relatively steady compared to the two-phase column referencing the probability density functions for both the liquid and bubble velocities. An analysis based on the determination of the drag forces and transversal lift forces was performed to examine the flow stability in the three-phase bubble column. The analysis illustrated that how the added solid phase effectively stabilized the flow field to achieve a steady circulation in the bubble column and a generalized criterion for the flow stability in the three-phase bubble column was derived. Further investigation for the transition and the heterogeneous bubble column regime with air rates at 2.0 and 4.0 L/min shown that this criterion can also be used as a general prediction of flow stability in this three-phase bubble column. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Phase Doppler anemometry was used to quantify the flow characteristic of a three phases (liquid, solid, and bubbles) cylindrical bubble column driven by a point air source made of a 30-mm diameter perforated air stone centrally mounted at the bottom. The cylindrical bubble column had an inner diameter of 152 mm and was filled with liquid up to 1 m above the point source. Acrylic beads with a nominal diameter of 3 mm were used as the solid phase. To match the density of the solid phase which was 1.05 kg/m3, the liquid density was raised to about 1.0485 kg/m3 by added salt. The bubble diameters generated were within the range of 600–2400 µm. The detailed turbulent characteristics of the liquid-phase velocity, bubble diameter, bubble velocity, and solid velocity were measured at three different air rates, namely 0.4, 0.8, and 1.2 L/min (corresponding to average gas volume fraction of 0.0084, 0.0168, and 0.0258, respectively) for the homogeneous bubble column regime. With the addition of the solid phase, the flow field was found to be relatively steady compared to the two-phase column referencing the probability density functions for both the liquid and bubble velocities. An analysis based on the determination of the drag forces and transversal lift forces was performed to examine the flow stability in the three-phase bubble column. The analysis illustrated that how the added solid phase effectively stabilized the flow field to achieve a steady circulation in the bubble column and a generalized criterion for the flow stability in the three-phase bubble column was derived. Further investigation for the transition and the heterogeneous bubble column regime with air rates at 2.0 and 4.0 L/min shown that this criterion can also be used as a general prediction of flow stability in this three-phase bubble column. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14036" xmlns="http://purl.org/rss/1.0/"><title>Residence time distribution in a single-phase rotor–stator spinning disk reactor</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14036</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Residence time distribution in a single-phase rotor–stator spinning disk reactor</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Frans Visscher, Jos Hullu, Mart H. J. M. Croon, John van der Schaaf, Jaap C. Schouten</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T11:48:27.568939-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14036</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14036</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14036</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena and Fluid Mechanics</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A reactor model for the single-phase rotor–stator spinning disk reactor based on residence time distribution measurements is described. For the experimental validation of the model, the axial clearance between the rotor and both stators is varied from 1.0 × 10<sup>−3</sup> to 3.0 × 10<sup>−3</sup> m, the rotational disk speed is varied from 50 to 2000 RPM, and the volumetric flow rate is varied from 7.5 × 10<sup>−6</sup> to 22.5 × 10<sup>−6</sup> m<sup>3</sup> s<sup>−1</sup>. Tracer injection experiments show that the residence time distribution can be described by a plug flow model in combination with 2–3 ideally stirred tanks-in-series. The resulting reactor model is explained with the effect of turbulence, the formation of Von Kármán and Bödewadt boundary layers, and the effect of the volumetric flow rate. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
A reactor model for the single-phase rotor–stator spinning disk reactor based on residence time distribution measurements is described. For the experimental validation of the model, the axial clearance between the rotor and both stators is varied from 1.0 × 10−3 to 3.0 × 10−3 m, the rotational disk speed is varied from 50 to 2000 RPM, and the volumetric flow rate is varied from 7.5 × 10−6 to 22.5 × 10−6 m3 s−1. Tracer injection experiments show that the residence time distribution can be described by a plug flow model in combination with 2–3 ideally stirred tanks-in-series. The resulting reactor model is explained with the effect of turbulence, the formation of Von Kármán and Bödewadt boundary layers, and the effect of the volumetric flow rate. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14045" xmlns="http://purl.org/rss/1.0/"><title>Modeling scale formation in flat-sheet membrane modules during water desalination</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14045</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Modeling scale formation in flat-sheet membrane modules during water desalination</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Margaritis Kostoglou, Anastasios J. Karabelas</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-22T13:01:27.316833-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14045</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14045</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14045</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separations: Materials, Devices and 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Modeling the operation of spiral-wound membrane modules is essential for their successful design and optimization. Such models must include the main types of membrane fouling, degrading desalination plant performance, including scaling due to sparingly soluble salts. Unfortunately, the complexity of underlying physicochemical processes and the coexistence of several spatial and temporal scales render intractable modeling of membrane scaling based on first principles. Therefore, a suitable (albeit simplified) framework is developed for incorporating scaling dynamics into a fluid flow model formulated at an intermediate (i.e., mesoscopic) length scale of membrane operation. The general mesoscopic approach involves integration of spatially distributed submodels, thereby allowing predictions at the large (entire membrane sheet) scale; these submodels comprise constitutive laws and kinetic rate expressions derived at fine scales. A submodel for the effect of pre-existing bulk particles on scale formation is developed herein. Several numerical results are presented to exemplify the potential of the proposed framework. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Modeling the operation of spiral-wound membrane modules is essential for their successful design and optimization. Such models must include the main types of membrane fouling, degrading desalination plant performance, including scaling due to sparingly soluble salts. Unfortunately, the complexity of underlying physicochemical processes and the coexistence of several spatial and temporal scales render intractable modeling of membrane scaling based on first principles. Therefore, a suitable (albeit simplified) framework is developed for incorporating scaling dynamics into a fluid flow model formulated at an intermediate (i.e., mesoscopic) length scale of membrane operation. The general mesoscopic approach involves integration of spatially distributed submodels, thereby allowing predictions at the large (entire membrane sheet) scale; these submodels comprise constitutive laws and kinetic rate expressions derived at fine scales. A submodel for the effect of pre-existing bulk particles on scale formation is developed herein. Several numerical results are presented to exemplify the potential of the proposed framework. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14038" xmlns="http://purl.org/rss/1.0/"><title>Direct catalytic upgrading of biomass pyrolysis vapors by a dual function Ru/TiO2 catalyst</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14038</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Direct catalytic upgrading of biomass pyrolysis vapors by a dual function Ru/TiO2 catalyst</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Shaolong Wan, Trung Pham, Sarah Zhang, Lance Lobban, Daniel Resasco, Richard Mallinson</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-22T13:01:15.055298-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14038</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14038</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14038</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Biomolecular Engineering, Bioengineering, Biochemicals, Biofuels, and Food</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The results of catalytic treatment of vapors exiting a g/min pyrolysis unit before product condensation to the liquid phase using a Ru/TiO<sub>2</sub> catalyst for oak and switchgrass pyrolysis are reported. The pyrolysis is conducted at 500°C and the catalysis at 400°C at atmospheric pressure with a hydrogen partial pressure of 0.58 atm. It is found that the catalytic treatment provides significant conversion of light oxygenates to larger, less oxygenated, molecules and, simultaneously, bio-oil phenolics are also converted to less oxygenated phenolics with methoxy methyl groups transferred to the ring. The activity of the catalyst gradually diminished with increasing biomass fed to the system. Untreated pyrolysis oil forms a single liquid phase with some tarry material, consistent with the literature, whereas the treated liquid product forms separate oil and aqueous phases, the latter of which is about 80% water. The oil from the treated vapors has a lower initial viscosity with only a small increase upon accelerated aging compared to the untreated product oil, which has a dramatic increase in viscosity after aging. This is indicative of poor oil stability for untreated oil that is further confirmed by large increases in molecular weight, while the treated oil has a small increase in molecular weight after accelerated aging. In an effort to understand compatibility with refinery streams, the solubility of the oils in tetralin was examined. The untreated oil was found to have very limited solubility in tetralin, whereas the treated oil phase was completely soluble except for a small aqueous phase that appeared. There are a number of challenges in developing a high yield process for pyrolysis based conversion of biomass to transportation fuels. The Ru/TiO<sub>2</sub> catalyst used here shows promise for conducting multiple types of favorable reactions in the presence of the full spectrum of primary pyrolysis products that creates significant product stability under mild conditions. This could lead to higher liquid yields of stable, refinery compatible, product oil. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The results of catalytic treatment of vapors exiting a g/min pyrolysis unit before product condensation to the liquid phase using a Ru/TiO2 catalyst for oak and switchgrass pyrolysis are reported. The pyrolysis is conducted at 500°C and the catalysis at 400°C at atmospheric pressure with a hydrogen partial pressure of 0.58 atm. It is found that the catalytic treatment provides significant conversion of light oxygenates to larger, less oxygenated, molecules and, simultaneously, bio-oil phenolics are also converted to less oxygenated phenolics with methoxy methyl groups transferred to the ring. The activity of the catalyst gradually diminished with increasing biomass fed to the system. Untreated pyrolysis oil forms a single liquid phase with some tarry material, consistent with the literature, whereas the treated liquid product forms separate oil and aqueous phases, the latter of which is about 80% water. The oil from the treated vapors has a lower initial viscosity with only a small increase upon accelerated aging compared to the untreated product oil, which has a dramatic increase in viscosity after aging. This is indicative of poor oil stability for untreated oil that is further confirmed by large increases in molecular weight, while the treated oil has a small increase in molecular weight after accelerated aging. In an effort to understand compatibility with refinery streams, the solubility of the oils in tetralin was examined. The untreated oil was found to have very limited solubility in tetralin, whereas the treated oil phase was completely soluble except for a small aqueous phase that appeared. There are a number of challenges in developing a high yield process for pyrolysis based conversion of biomass to transportation fuels. The Ru/TiO2 catalyst used here shows promise for conducting multiple types of favorable reactions in the presence of the full spectrum of primary pyrolysis products that creates significant product stability under mild conditions. This could lead to higher liquid yields of stable, refinery compatible, product oil. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14035" xmlns="http://purl.org/rss/1.0/"><title>Pressure drop in a split-and-recombine caterpillar micromixer in case of newtonian and non-newtonian fluids</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14035</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Pressure drop in a split-and-recombine caterpillar micromixer in case of newtonian and non-newtonian fluids</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Odile Carrier, Denis Funfschilling, Hélène Debas, Souhila Poncin, Patrick Löb, Huai-Zhi Li</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-22T12:39:26.184682-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14035</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14035</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14035</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena and Fluid Mechanics</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Microreactors are very promising tools for the design of future chemical processes. For example, emulsions of very narrow size distribution are obtained at much lower energy consumption than the one spent with usual processes. Micromixers play thereby an eminent role. The goal of this study is to better understand the hydrodynamic properties of a split-and-recombine Caterpillar micromixer (CPMM) specially with regard to handling viscoelastic fluids, a topic hardly addressed so far in the context of micromixers in general, although industrial fluids like detergent, cosmetic, or food emulsions are non-Newtonian. Friction factor was measured in a CPMM for both Newtonian and non-Newtonian fluids. For Newtonian fluids, the friction factor in the laminar regime is f/2 = 24/Re. The laminar regime exists up to Reynolds numbers of 15. For shear-thinning fluids like Carbopol 940 or viscoelastic fluids like Poly Acryl Amide (PAAm) aqueous solutions, the friction factor scales identically within statistical errors up to a generalized Reynolds number of 10 and 0.01, respectively. Above that limit, there is an excess pressure drop for the viscoelastic PAAm solution. This excess pressure drop multiplies the friction factor by more than a decade over a decade of Reynolds numbers. The origin of this excess pressure drop is the high elongational flow present in the Caterpillar static mixer applied to a highly viscoelastic fluid. This result can be extended to almost all static mixers, because their flows are generally highly elongational. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Microreactors are very promising tools for the design of future chemical processes. For example, emulsions of very narrow size distribution are obtained at much lower energy consumption than the one spent with usual processes. Micromixers play thereby an eminent role. The goal of this study is to better understand the hydrodynamic properties of a split-and-recombine Caterpillar micromixer (CPMM) specially with regard to handling viscoelastic fluids, a topic hardly addressed so far in the context of micromixers in general, although industrial fluids like detergent, cosmetic, or food emulsions are non-Newtonian. Friction factor was measured in a CPMM for both Newtonian and non-Newtonian fluids. For Newtonian fluids, the friction factor in the laminar regime is f/2 = 24/Re. The laminar regime exists up to Reynolds numbers of 15. For shear-thinning fluids like Carbopol 940 or viscoelastic fluids like Poly Acryl Amide (PAAm) aqueous solutions, the friction factor scales identically within statistical errors up to a generalized Reynolds number of 10 and 0.01, respectively. Above that limit, there is an excess pressure drop for the viscoelastic PAAm solution. This excess pressure drop multiplies the friction factor by more than a decade over a decade of Reynolds numbers. The origin of this excess pressure drop is the high elongational flow present in the Caterpillar static mixer applied to a highly viscoelastic fluid. This result can be extended to almost all static mixers, because their flows are generally highly elongational. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14030" xmlns="http://purl.org/rss/1.0/"><title>Multiobjective optimization of biorefineries with economic and safety objectives</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14030</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Multiobjective optimization of biorefineries with economic and safety objectives</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ali M. El-Halwagi, Camilo Rosas, José María Ponce-Ortega, Arturo Jiménez-Gutiérrez, Mahboobul S. Mannan, Mahmoud M. El-Halwagi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-22T11:44:50.415303-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14030</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14030</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14030</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A new approach for the incorporation of safety criteria into the selection, location, and sizing of a biorefinery is introduced. In addition to the techno-economic factors, risk metrics are used in the decision-making process by considering the cumulative risk associated with key stages of the life cycle of a biorefinery that includes biomass storage and transportation, process conversion into biofuels or bioproducts, and product storage. The fixed cost of the process along with the operating costs for transportation and processing as well as the value of the product are included. An optimization formulation is developed based on a superstructure that embeds potential supply chains of interest. The optimization program establishes the tradeoffs between cost and safety issues in the form of Pareto curves. A case study on bio-hydrogen production is solved to illustrate the merits of the proposed approach. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
A new approach for the incorporation of safety criteria into the selection, location, and sizing of a biorefinery is introduced. In addition to the techno-economic factors, risk metrics are used in the decision-making process by considering the cumulative risk associated with key stages of the life cycle of a biorefinery that includes biomass storage and transportation, process conversion into biofuels or bioproducts, and product storage. The fixed cost of the process along with the operating costs for transportation and processing as well as the value of the product are included. An optimization formulation is developed based on a superstructure that embeds potential supply chains of interest. The optimization program establishes the tradeoffs between cost and safety issues in the form of Pareto curves. A case study on bio-hydrogen production is solved to illustrate the merits of the proposed approach. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14028" xmlns="http://purl.org/rss/1.0/"><title>Economic Plantwide Control Over a Wide Throughput Range: A Systematic Design Procedure</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14028</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Economic Plantwide Control Over a Wide Throughput Range: A Systematic Design Procedure</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Rahul Jagtap, Nitin Kaistha, Sigurd Skogestad</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-20T14:55:37.835904-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14028</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14028</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14028</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A systematic top-down procedure to design an effective plantwide control system for economically (near) optimum process operation over a wide throughput range is developed. The proposed procedure focuses on devising a control system for optimal operation at maximum throughput, where usually the highest number of constraints is active and the economic benefits of improved operation are the greatest. To do so, loops for tight control of all the active constraints and economically sound controlled variables (CVs) corresponding to unconstrained degrees of freedom are first implemented (Step 1) followed by a consistent inventory control system (Step 2). This control system is adapted with setpoints that become unconstrained at lower throughputs taking up additional economic CV control or throughput manipulation (Step 3). Iteration between the three steps may be necessary to eliminate fragile/unconventional inventory loops (Step 4). The application of the methodology is demonstrated on three realistic example processes. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
A systematic top-down procedure to design an effective plantwide control system for economically (near) optimum process operation over a wide throughput range is developed. The proposed procedure focuses on devising a control system for optimal operation at maximum throughput, where usually the highest number of constraints is active and the economic benefits of improved operation are the greatest. To do so, loops for tight control of all the active constraints and economically sound controlled variables (CVs) corresponding to unconstrained degrees of freedom are first implemented (Step 1) followed by a consistent inventory control system (Step 2). This control system is adapted with setpoints that become unconstrained at lower throughputs taking up additional economic CV control or throughput manipulation (Step 3). Iteration between the three steps may be necessary to eliminate fragile/unconventional inventory loops (Step 4). The application of the methodology is demonstrated on three realistic example processes. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14017" xmlns="http://purl.org/rss/1.0/"><title>Catalytic Activity of Cu/SBA-15 for Peroxidation of Pyridine Bearing Wastewater at Atmospheric Condition</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14017</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Catalytic Activity of Cu/SBA-15 for Peroxidation of Pyridine Bearing Wastewater at Atmospheric Condition</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">V. Subbaramaiah, Vimal Chandra Srivastava, Indra Deo Mall</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-19T16:39:55.341599-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14017</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14017</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14017</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>In this study, Cu-loaded Santa Barbara amorphous (SBA)-15 catalysts were synthesized by impregnation method and further used for catalytic wet peroxidation (CWPO) of pyridine from aqueous solution using hydrogen peroxide as oxidant. The synthesized catalysts have been characterized by Brunauer–Emmett–Teller surface area: temperature-programmed reduction, H<sub>2</sub>-chemisorption, Fourier transform infrared spectroscopy, and field emission scanning electron microscopy. Characterization results indicate good dispersion of Cu species inside the porous structure of SBA-15. The effect of various parameters such as Cu loading on SBA-15, pH, catalyst dose, H<sub>2</sub>O<sub>2</sub> concentration, and temperature have been studied for their effect on CWPO of pyridine. More than 97% pyridine removal and 92% total organic carbon removal was achieved at optimum condition. Cu/SBA-15 showed stable performance during reuse for six cycles with negligible copper leaching. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
In this study, Cu-loaded Santa Barbara amorphous (SBA)-15 catalysts were synthesized by impregnation method and further used for catalytic wet peroxidation (CWPO) of pyridine from aqueous solution using hydrogen peroxide as oxidant. The synthesized catalysts have been characterized by Brunauer–Emmett–Teller surface area: temperature-programmed reduction, H2-chemisorption, Fourier transform infrared spectroscopy, and field emission scanning electron microscopy. Characterization results indicate good dispersion of Cu species inside the porous structure of SBA-15. The effect of various parameters such as Cu loading on SBA-15, pH, catalyst dose, H2O2 concentration, and temperature have been studied for their effect on CWPO of pyridine. More than 97% pyridine removal and 92% total organic carbon removal was achieved at optimum condition. Cu/SBA-15 showed stable performance during reuse for six cycles with negligible copper leaching. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14009" xmlns="http://purl.org/rss/1.0/"><title>Ionic Liquid Confined in Nafion: Toward Molecular-Level Understanding</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14009</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Ionic Liquid Confined in Nafion: Toward Molecular-Level Understanding</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Delin Sun, Jian Zhou</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-19T16:15:45.569521-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14009</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14009</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14009</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Thermodynamics and Molecular-Scale 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>In this article, multiscale simulation methods were used to study structural and transport properties of Nafion–ionic liquid composite membranes that are novel proton conducting materials for fuel cells. Coarse-grained model for 1-butyl-3-methylimidazolium tetrafluoroborate ([bmim][BF<sub>4</sub>]) ionic liquid was first developed in the framework of BMW-MARTINI force field. Coarse-grained simulation results of bulk [bmim][BF<sub>4</sub>] ionic liquid show good agreement with all-atom simulation results and experimental data. Nafion–[bmim][BF<sub>4</sub>] composite membranes were then simulated using all-atom and coarse-grained models. Ionic liquid cluster formation inside Nafion was revealed by coarse-grained simulations. Diffusion coefficients of both [bmim]<sup>+</sup> cations and 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/aic.14009/asset/equation/aic14009-math-0001.gif?v=1&amp;t=hh0j2kh3&amp;s=e73bc6b8d66fa2a87c09ea85b6a312148c68f476" class="inlineGraphic"/> anions are reduced by one to two orders of magnitude depending on their concentrations in Nafion membrane. [Bmim]<sup>+</sup> cations have faster self-diffusion coefficient than 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/aic.14009/asset/equation/aic14009-math-0002.gif?v=1&amp;t=hh0j2kh4&amp;s=94a3ca3d9738a4bd793674372930d898878648c5" class="inlineGraphic"/> anions, while this phenomenon is more pronounced when ionic liquids are confined in Nafion. This work provides molecular basis for understanding Nafion–ionic liquid composite membranes. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
In this article, multiscale simulation methods were used to study structural and transport properties of Nafion–ionic liquid composite membranes that are novel proton conducting materials for fuel cells. Coarse-grained model for 1-butyl-3-methylimidazolium tetrafluoroborate ([bmim][BF4]) ionic liquid was first developed in the framework of BMW-MARTINI force field. Coarse-grained simulation results of bulk [bmim][BF4] ionic liquid show good agreement with all-atom simulation results and experimental data. Nafion–[bmim][BF4] composite membranes were then simulated using all-atom and coarse-grained models. Ionic liquid cluster formation inside Nafion was revealed by coarse-grained simulations. Diffusion coefficients of both [bmim]+ cations and 
BF4− anions are reduced by one to two orders of magnitude depending on their concentrations in Nafion membrane. [Bmim]+ cations have faster self-diffusion coefficient than 
BF4− anions, while this phenomenon is more pronounced when ionic liquids are confined in Nafion. This work provides molecular basis for understanding Nafion–ionic liquid composite membranes. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14011" xmlns="http://purl.org/rss/1.0/"><title>Role of Guest Molecules on the Hydrate Growth at Vapor-Liquid Interfaces</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14011</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Role of Guest Molecules on the Hydrate Growth at Vapor-Liquid Interfaces</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dongsheng Bai, Bei Liu, Guangjin Chen, Xianren Zhang, Wenchuan Wang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-14T08:54:12.671668-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14011</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14011</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14011</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Thermodynamics and Molecular-Scale 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Systematic molecular dynamics simulations have been performed to illustrate the roles of guest molecules played in the process of hydrate growth at vapor-liquid interfaces. In our simulations, guest molecules are represented by a commonly used single-site Lennard–Jones model, and the roles of guest molecules on hydrate growth have been investigated separately from the effect of water–guest molecule attractive interaction ε and that of molecular size σ, respectively. Our simulation results demonstrate that the water-guest molecule attraction regulates the pathway and rate of nucleus growth, whereas the size of guest molecules determines the dynamically preferable structure. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Systematic molecular dynamics simulations have been performed to illustrate the roles of guest molecules played in the process of hydrate growth at vapor-liquid interfaces. In our simulations, guest molecules are represented by a commonly used single-site Lennard–Jones model, and the roles of guest molecules on hydrate growth have been investigated separately from the effect of water–guest molecule attractive interaction ε and that of molecular size σ, respectively. Our simulation results demonstrate that the water-guest molecule attraction regulates the pathway and rate of nucleus growth, whereas the size of guest molecules determines the dynamically preferable structure. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14026" xmlns="http://purl.org/rss/1.0/"><title>Catalytic Methanation of Carbon Dioxide by Active Oxygen Material CexZr1−xO2 Supported Ni<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>Co Bimetallic Nanocatalysts</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14026</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Catalytic Methanation of Carbon Dioxide by Active Oxygen Material CexZr1−xO2 Supported Ni<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>Co Bimetallic Nanocatalysts</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hongwei Zhu, Rauf Razzaq, Chunshan Li, Yaseen Muhmmad, Suojiang Zhang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-14T08:45:29.074304-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14026</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14026</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14026</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A series of active oxygen material Ce<sub>x</sub>Zr<sub>1−x</sub>O<sub>2</sub>-supported Ni<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>Co bimetallic nanosized catalysts were prepared by coprecipitation method, which is simple and fit for industrial use with lower cost than other methods. The effect of CeO<sub>2</sub>/ZrO<sub>2</sub> mole ratio, Co metal addition, and PEG-6000 addition were investigated. The catalysts were characterized through X-ray diffraction, H<sub>2</sub> thermal-programmed reduction, N<sub>2</sub> adsorption, Raman spectroscopy, CO pulse chemisorption, X-ray photoelectron spectroscopy, oxygen storage capacity, and transmission electron microscopy-energy dispersive X-ray analysis. Modifications of the structural and redox properties of these materials were evaluated in relation to their catalytic performances. Particularly, the relationship between the active oxygen sites of the catalysts and their catalytic performances was investigated. The interaction between active metals (Ni and Co) and Ce<sub>x</sub>Zr<sub>1−x</sub>O<sub>2</sub> support was found to be very important for catalytic performance. The active oxygen site of Ce<sub>x</sub>Zr<sub>1−x</sub>O<sub>2</sub> can considerably improve catalytic performance. Appropriate Co metal addition also remarkably enhanced the catalytic stability and activity. Moreover, PEG-6000 addition can improve the Brunauer–Emmett–Teller surface area and active metal dispersion of catalysts to improve their performances. The nanosized catalyst 15 wt % Ni-5 wt % Co/Ce<sub>0.25</sub>Zr<sub>0.75</sub>O<sub>2</sub> prepared by adding 5 wt % PEG-6000 achieved almost 85% CO<sub>2</sub> conversion and 98% selectivity to methane at 280°C when the gas hourly space velocity was 10,000 h<sup>−1</sup>. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
A series of active oxygen material CexZr1−xO2-supported Ni<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>Co bimetallic nanosized catalysts were prepared by coprecipitation method, which is simple and fit for industrial use with lower cost than other methods. The effect of CeO2/ZrO2 mole ratio, Co metal addition, and PEG-6000 addition were investigated. The catalysts were characterized through X-ray diffraction, H2 thermal-programmed reduction, N2 adsorption, Raman spectroscopy, CO pulse chemisorption, X-ray photoelectron spectroscopy, oxygen storage capacity, and transmission electron microscopy-energy dispersive X-ray analysis. Modifications of the structural and redox properties of these materials were evaluated in relation to their catalytic performances. Particularly, the relationship between the active oxygen sites of the catalysts and their catalytic performances was investigated. The interaction between active metals (Ni and Co) and CexZr1−xO2 support was found to be very important for catalytic performance. The active oxygen site of CexZr1−xO2 can considerably improve catalytic performance. Appropriate Co metal addition also remarkably enhanced the catalytic stability and activity. Moreover, PEG-6000 addition can improve the Brunauer–Emmett–Teller surface area and active metal dispersion of catalysts to improve their performances. The nanosized catalyst 15 wt % Ni-5 wt % Co/Ce0.25Zr0.75O2 prepared by adding 5 wt % PEG-6000 achieved almost 85% CO2 conversion and 98% selectivity to methane at 280°C when the gas hourly space velocity was 10,000 h−1. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14023" xmlns="http://purl.org/rss/1.0/"><title>Fluctuations, Order, and Disorder in Short Diblock Copolymers</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14023</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Fluctuations, Order, and Disorder in Short Diblock Copolymers</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sangwoo Lee, Timothy M. Gillard, Frank S. Bates</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-11T17:57:00.48671-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14023</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14023</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14023</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. Thermodynamics and Molecular-Scale 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The phase behavior for a series of poly(1,4-isoprene-b-DL-lactide) diblock copolymers characterized by a relatively large Flory–Huggins segment–segment interaction parameter (χ) and low degrees of polymerization (N) over a range of compositions was reported. Ordered-state morphologies were deduced from small-angle x-ray scattering (SAXS) measurements, and χ(T) was determined from order-disorder transition temperatures (T<sub>ODT</sub>'s) associated with the compositionally symmetric specimens and assuming the mean-field theory, that is, (χN)<sub>ODT</sub>=10.5. The ODT was determined by differential scanning calorimetry, SAXS, and dynamic mechanical spectroscopy, and shown to be weakly first-order, with latent heats of transition that vary strongly with composition. We interpret this behavior in terms of the mean and Gauss interfacial curvature of the ordered-state morphologies and with respect to composition fluctuations in the disordered state. These results offer a fresh strategy for investigating weakly first-order phase transitions within the Brazovskii universality class. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The phase behavior for a series of poly(1,4-isoprene-b-DL-lactide) diblock copolymers characterized by a relatively large Flory–Huggins segment–segment interaction parameter (χ) and low degrees of polymerization (N) over a range of compositions was reported. Ordered-state morphologies were deduced from small-angle x-ray scattering (SAXS) measurements, and χ(T) was determined from order-disorder transition temperatures (TODT's) associated with the compositionally symmetric specimens and assuming the mean-field theory, that is, (χN)ODT=10.5. The ODT was determined by differential scanning calorimetry, SAXS, and dynamic mechanical spectroscopy, and shown to be weakly first-order, with latent heats of transition that vary strongly with composition. We interpret this behavior in terms of the mean and Gauss interfacial curvature of the ordered-state morphologies and with respect to composition fluctuations in the disordered state. These results offer a fresh strategy for investigating weakly first-order phase transitions within the Brazovskii universality class. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14022" xmlns="http://purl.org/rss/1.0/"><title>Integrated Scheduling and Dynamic Optimization of Sequential Batch Processes with Online Implementation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14022</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Integrated Scheduling and Dynamic Optimization of Sequential Batch Processes with Online Implementation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yunfei Chu, Fengqi You</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-07T14:12:20.539125-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14022</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14022</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14022</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>An efficient decomposition method to solve the integrated problem of scheduling and dynamic optimization for sequential batch processes is proposed. The integrated problem is formulated as a mixed-integer dynamic optimization problem or a large-scale mixed-integer nonlinear programming (MINLP) problem by discretizing the dynamic models. To reduce the computational complexity, we first decompose all dynamic models from the integrated problem, which is then approximated by a scheduling problem based on the flexible recipe. The recipe candidates are expressed by Pareto frontiers, which are determined offline by using multiobjective dynamic optimization to minimize the processing cost and processing time. The operational recipe is then optimized simultaneously with the scheduling decisions online. Because the dynamic models are encapsulated by the Pareto frontiers, the online problem is a mixed-integer programming problem which is much more computationally efficient than the original MINLP problem, and allows the online implementation to deal with uncertainties. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
An efficient decomposition method to solve the integrated problem of scheduling and dynamic optimization for sequential batch processes is proposed. The integrated problem is formulated as a mixed-integer dynamic optimization problem or a large-scale mixed-integer nonlinear programming (MINLP) problem by discretizing the dynamic models. To reduce the computational complexity, we first decompose all dynamic models from the integrated problem, which is then approximated by a scheduling problem based on the flexible recipe. The recipe candidates are expressed by Pareto frontiers, which are determined offline by using multiobjective dynamic optimization to minimize the processing cost and processing time. The operational recipe is then optimized simultaneously with the scheduling decisions online. Because the dynamic models are encapsulated by the Pareto frontiers, the online problem is a mixed-integer programming problem which is much more computationally efficient than the original MINLP problem, and allows the online implementation to deal with uncertainties. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14018" xmlns="http://purl.org/rss/1.0/"><title>Continuum model validation of gas jet plume injection into a gas–solid bubbling fluidized bed</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14018</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Continuum model validation of gas jet plume injection into a gas–solid bubbling fluidized bed</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Deepak Rangarajan, Jennifer S. Curtis, Sofiane Benyahia, Alexander G. Mychkovsky</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-31T15:57:09.501069-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14018</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14018</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14018</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. Particle Technology and Fluidization</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A continuum gas–solid model that includes descriptions for solid frictional stress and a turbulent gas phase is evaluated against published experimental measurements of mean and fluctuating velocity inside the jet plume region of a bubbling fluidized bed with a high-speed vertical jet injection. The main uncertainties in closure relations necessary in the continuum model are first identified and then determined using available experimental data. The overall model shows good agreement with both the gas and particle experimental velocity profiles. The trends in the centerline mean and fluctuating velocity with change in the fluidized state of the emulsion are also captured favorably. Main deviations between the model and experiment are noted and possible reasons for the mismatch are discussed. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
A continuum gas–solid model that includes descriptions for solid frictional stress and a turbulent gas phase is evaluated against published experimental measurements of mean and fluctuating velocity inside the jet plume region of a bubbling fluidized bed with a high-speed vertical jet injection. The main uncertainties in closure relations necessary in the continuum model are first identified and then determined using available experimental data. The overall model shows good agreement with both the gas and particle experimental velocity profiles. The trends in the centerline mean and fluctuating velocity with change in the fluidized state of the emulsion are also captured favorably. Main deviations between the model and experiment are noted and possible reasons for the mismatch are discussed. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14001" xmlns="http://purl.org/rss/1.0/"><title>Guaranteed cost distributed fuzzy observer-based control for a class of nonlinear spatially distributed processes</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14001</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Guaranteed cost distributed fuzzy observer-based control for a class of nonlinear spatially distributed processes</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jun-Wei Wang, Huai-Ning Wu, Han-Xiong Li</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-30T10:30:36.040951-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14001</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14001</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14001</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The guaranteed cost distributed fuzzy (GCDF) observer-based control design is proposed for a class of nonlinear spatially distributed processes described by first-order hyperbolic partial differential equations (PDEs). Initially, a T–S fuzzy hyperbolic PDE model is proposed to accurately represent the nonlinear PDE system. Then, based on the fuzzy PDE model, the GCDF observer-based control design is developed in terms of a set of space-dependent linear matrix inequalities. In the proposed control scheme, a distributed fuzzy observer is used to estimate the state of the PDE system. The designed fuzzy controller can not only ensure the exponential stability of the closed-loop PDE system but also provide an upper bound of quadratic cost function. Moreover, a suboptimal fuzzy control design is addressed in the sense of minimizing an upper bound of the cost function. The finite difference method in space and the existing linear matrix inequality optimization techniques are used to approximately solve the suboptimal control design problem. Finally, the proposed design method is applied to the control of a nonisothermal plug-flow reactor. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The guaranteed cost distributed fuzzy (GCDF) observer-based control design is proposed for a class of nonlinear spatially distributed processes described by first-order hyperbolic partial differential equations (PDEs). Initially, a T–S fuzzy hyperbolic PDE model is proposed to accurately represent the nonlinear PDE system. Then, based on the fuzzy PDE model, the GCDF observer-based control design is developed in terms of a set of space-dependent linear matrix inequalities. In the proposed control scheme, a distributed fuzzy observer is used to estimate the state of the PDE system. The designed fuzzy controller can not only ensure the exponential stability of the closed-loop PDE system but also provide an upper bound of quadratic cost function. Moreover, a suboptimal fuzzy control design is addressed in the sense of minimizing an upper bound of the cost function. The finite difference method in space and the existing linear matrix inequality optimization techniques are used to approximately solve the suboptimal control design problem. Finally, the proposed design method is applied to the control of a nonisothermal plug-flow reactor. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14008" xmlns="http://purl.org/rss/1.0/"><title>Conversion of isopropanol and mixed alcohols to hydrocarbons using HZSM-5 Catalyst in the MixAlco™ process</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14008</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Conversion of isopropanol and mixed alcohols to hydrocarbons using HZSM-5 Catalyst in the MixAlco™ process</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sebastian Taco-Vasquez, Mark T. Holtzapple</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-28T21:49:17.288004-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14008</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14008</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14008</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>HZSM-5 (SiO<sub>2</sub>/Al<sub>2</sub>O<sub>3</sub>=280 mol/mol) is used to produce hydrocarbons from reagent-grade isopropanol and mixed alcohols made from lignocellulosic biomass (waste office paper and chicken manure) using the MixAlco™ process. All studies were performed at 101 kPa (abs). The experiments were conducted in two sets: (1) vary temperature (300–T<sub>max</sub>°C) at weight hourly space velocity (WHSV)=1.31 h<sup>–1</sup>, and (2) vary WHSV (0.5–11.5 h<sup>–1</sup>) at T=370°C. For isopropanol, T<sub>max</sub>=450°C and for mixed alcohols T<sub>max</sub>=520°C. For isopropanol, higher temperatures produced more gaseous products and more aromatics. High WHSV gives high concentration of C6+ olefins, whereas low WHSV gives high concentrations of C9 aromatics. For mixed alcohols, changes in temperature affected the product distribution similar to isopropanol. In contrast, WHSV did not affect the concentration of reaction products; only dehydration products were observed. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
HZSM-5 (SiO2/Al2O3=280 mol/mol) is used to produce hydrocarbons from reagent-grade isopropanol and mixed alcohols made from lignocellulosic biomass (waste office paper and chicken manure) using the MixAlco™ process. All studies were performed at 101 kPa (abs). The experiments were conducted in two sets: (1) vary temperature (300–Tmax°C) at weight hourly space velocity (WHSV)=1.31 h–1, and (2) vary WHSV (0.5–11.5 h–1) at T=370°C. For isopropanol, Tmax=450°C and for mixed alcohols Tmax=520°C. For isopropanol, higher temperatures produced more gaseous products and more aromatics. High WHSV gives high concentration of C6+ olefins, whereas low WHSV gives high concentrations of C9 aromatics. For mixed alcohols, changes in temperature affected the product distribution similar to isopropanol. In contrast, WHSV did not affect the concentration of reaction products; only dehydration products were observed. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14019" xmlns="http://purl.org/rss/1.0/"><title>High yield production and purification of 5-hydroxymethylfurfural</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14019</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">High yield production and purification of 5-hydroxymethylfurfural</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jianjian Wang, Jiawen Ren, Xiaohui Liu, Guanzhong Lu, Yanqin Wang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-28T21:23:11.241521-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14019</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14019</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14019</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Conversion of carbohydrates to 5-hydroxymethylfurfural (HMF) will provide a new step toward achieving renewable biomass-based chemicals and fuels platform. Recently, the excellent yield of HMF (91.0%) in dimethyl sulfoxide (DMSO) catalyzed by sulfonated carbon was demonstrated, but the separation of HMF from the reaction mixture remains challenging because of the high boiling point of DMSO. As a solution, herein, low boiling point solvent tetrahydrofuran (THF) mixed with DMSO was used for the fructose dehydration and high yield of HMF (98.0%) was still obtained. Besides, the stability of the sulfonated carbonaceous catalyst was also confirmed. More importantly, HMF from the reaction solution was successfully separated by using simple extraction method, and high purity of HMF (ca. 96.4%) was obtained. Compared with pure DMSO solvent, the combination of low boiling point THF with DMSO not only gives higher yield of HMF, but also improves the separation efficiency and reduces environmental risk. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Conversion of carbohydrates to 5-hydroxymethylfurfural (HMF) will provide a new step toward achieving renewable biomass-based chemicals and fuels platform. Recently, the excellent yield of HMF (91.0%) in dimethyl sulfoxide (DMSO) catalyzed by sulfonated carbon was demonstrated, but the separation of HMF from the reaction mixture remains challenging because of the high boiling point of DMSO. As a solution, herein, low boiling point solvent tetrahydrofuran (THF) mixed with DMSO was used for the fructose dehydration and high yield of HMF (98.0%) was still obtained. Besides, the stability of the sulfonated carbonaceous catalyst was also confirmed. More importantly, HMF from the reaction solution was successfully separated by using simple extraction method, and high purity of HMF (ca. 96.4%) was obtained. Compared with pure DMSO solvent, the combination of low boiling point THF with DMSO not only gives higher yield of HMF, but also improves the separation efficiency and reduces environmental risk. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14016" xmlns="http://purl.org/rss/1.0/"><title>Beyond shape selective catalysis with zeolites: Hydrophobic void spaces in zeolites enable catalysis in liquid water</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14016</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Beyond shape selective catalysis with zeolites: Hydrophobic void spaces in zeolites enable catalysis in liquid water</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Rajamani Gounder, Mark E. Davis</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-24T14:43:10.399389-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14016</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14016</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14016</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. Reaction Engineering, 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Zeolites confine active sites within void spaces of molecular dimension. The size and shape of these voids can be tuned by changing framework topology, which can influence catalytic reactivity and selectivity via coupled reaction-transport phenomena that exploit differences in transport properties among reactants and/or products that differ in size and shape. The polarity and solvating properties of intrazeolite void environments can be tuned by changing chemical composition and structure, ranging from hydrophobic defect-free pure-silica surfaces to silica surfaces containing hydrophilic defect sites and/or heteroatoms. Here, we discuss how the polarity of zeolite voids influences catalytic reactivity and selectivity via the partitioning of reactant, product, and solvent molecules between intrazeolitic locations and external fluid phases. These findings provide a conceptual basis for developing selective catalytic processes in aqueous media using hydrophobic zeolites that are able to adsorb organic reactants while excluding liquid water from internal void spaces. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Zeolites confine active sites within void spaces of molecular dimension. The size and shape of these voids can be tuned by changing framework topology, which can influence catalytic reactivity and selectivity via coupled reaction-transport phenomena that exploit differences in transport properties among reactants and/or products that differ in size and shape. The polarity and solvating properties of intrazeolite void environments can be tuned by changing chemical composition and structure, ranging from hydrophobic defect-free pure-silica surfaces to silica surfaces containing hydrophilic defect sites and/or heteroatoms. Here, we discuss how the polarity of zeolite voids influences catalytic reactivity and selectivity via the partitioning of reactant, product, and solvent molecules between intrazeolitic locations and external fluid phases. These findings provide a conceptual basis for developing selective catalytic processes in aqueous media using hydrophobic zeolites that are able to adsorb organic reactants while excluding liquid water from internal void spaces. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14015" xmlns="http://purl.org/rss/1.0/"><title>CaCO3 fouling on microscale–nanoscale hydrophobic titania–fluoroalkylsilane films in pool boiling</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14015</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">CaCO3 fouling on microscale–nanoscale hydrophobic titania–fluoroalkylsilane films in pool boiling</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yongwei Cai, Mingyan Liu, Longfei Hui</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-24T12:45:58.826565-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14015</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14015</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14015</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena and Fluid Mechanics</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Micrometer–nanometer hydrophobic titania–fluoroalkylsilane composite coatings were prepared on substrates based on liquid-phase deposition. Coatings and crystallization forms were characterized with instruments of surface analyses. Experimental facilities of pool boiling were established to evaluate heat and mass transfer on coated surfaces in deionized water and saturated calcium carbonate solution. Obvious pool boiling enhancement was observed on thinner microscale–nanoscale hydrophobic titania–fluoroalkylsilane composite films at higher heat fluxes compared to that on thicker titania–fluoroalkylsilane coatings or on titania coatings and stainless steel surfaces. Lower fouling resistance was obtained on titania–fluoroalkylsilane coatings in pool boiling of saturated calcium carbonate solution and crystal form was aragonite, which was different from calcite on titania coatings. Results of inhibition of fouling and enhancement of heat transfer on titania–fluoroalkylsilane coatings were contributed to special surface microscale–nanoscale structure and material wettability. Asymptotic model was used to fit experimental data of fouling resistance, and reasonable agreement was obtained. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Micrometer–nanometer hydrophobic titania–fluoroalkylsilane composite coatings were prepared on substrates based on liquid-phase deposition. Coatings and crystallization forms were characterized with instruments of surface analyses. Experimental facilities of pool boiling were established to evaluate heat and mass transfer on coated surfaces in deionized water and saturated calcium carbonate solution. Obvious pool boiling enhancement was observed on thinner microscale–nanoscale hydrophobic titania–fluoroalkylsilane composite films at higher heat fluxes compared to that on thicker titania–fluoroalkylsilane coatings or on titania coatings and stainless steel surfaces. Lower fouling resistance was obtained on titania–fluoroalkylsilane coatings in pool boiling of saturated calcium carbonate solution and crystal form was aragonite, which was different from calcite on titania coatings. Results of inhibition of fouling and enhancement of heat transfer on titania–fluoroalkylsilane coatings were contributed to special surface microscale–nanoscale structure and material wettability. Asymptotic model was used to fit experimental data of fouling resistance, and reasonable agreement was obtained. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14014" xmlns="http://purl.org/rss/1.0/"><title>Global approximations of unsteady-state adsorption, diffusion, and reaction in a porous catalyst</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14014</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Global approximations of unsteady-state adsorption, diffusion, and reaction in a porous catalyst</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jietae Lee, Dong Hyun Kim</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-24T09:16:45.438876-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14014</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14014</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14014</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The pore diffusion model that describes unsteady-state adsorption, diffusion, and reaction in a porous catalyst is in the form of a parabolic partial differential equation. To relieve computational loads, approximate ordinary differential equations are often used and they can be derived from the transfer function between the surface and average concentrations in the particle. The transfer function shows half-order behaviors at the high-frequency range. The rational transfer functions cannot describe well this half-order behavior. Here, introducing the half-order term to rational transfer function candidates for approximation, models valid throughout low- and high-frequency ranges are derived. Since the proposed approximate models are valid globally, they can be applied to reactive porous catalysts easily. They can also be used for noninteger shape factors that will show better performances for adsorbents different from ideal geometries of infinite slab, infinite cylinder and sphere, and for biporous adsorbents. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The pore diffusion model that describes unsteady-state adsorption, diffusion, and reaction in a porous catalyst is in the form of a parabolic partial differential equation. To relieve computational loads, approximate ordinary differential equations are often used and they can be derived from the transfer function between the surface and average concentrations in the particle. The transfer function shows half-order behaviors at the high-frequency range. The rational transfer functions cannot describe well this half-order behavior. Here, introducing the half-order term to rational transfer function candidates for approximation, models valid throughout low- and high-frequency ranges are derived. Since the proposed approximate models are valid globally, they can be applied to reactive porous catalysts easily. They can also be used for noninteger shape factors that will show better performances for adsorbents different from ideal geometries of infinite slab, infinite cylinder and sphere, and for biporous adsorbents. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14013" xmlns="http://purl.org/rss/1.0/"><title>A novel dynamic bayesian network-based networked process monitoring approach for fault detection, propagation identification, and root cause diagnosis</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14013</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A novel dynamic bayesian network-based networked process monitoring approach for fault detection, propagation identification, and root cause diagnosis</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jie Yu, Mudassir M. Rashid</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-24T08:58:44.640339-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14013</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14013</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14013</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A novel networked process monitoring, fault propagation identification, and root cause diagnosis approach is developed in this study. First, process network structure is determined from prior process knowledge and analysis. The network model parameters including the conditional probability density functions of different nodes are then estimated from process operating data to characterize the causal relationships among the monitored variables. Subsequently, the Bayesian inference-based abnormality likelihood index is proposed to detect abnormal events in chemical processes. After the process fault is detected, the novel dynamic Bayesian probability and contribution indices are further developed from the transitional probabilities of monitored variables to identify the major faulty effect variables with significant upsets. With the dynamic Bayesian contribution index, the statistical inference rules are, thus, designed to search for the fault propagation pathways from the downstream backwards to the upstream process. In this way, the ending nodes in the identified propagation pathways can be captured as the root cause variables of process faults. Meanwhile, the identified fault propagation sequence provides an in-depth understanding as to the interactive effects of faults throughout the processes. The proposed approach is demonstrated using the illustrative continuous stirred tank reactor system and the Tennessee Eastman chemical process with the fault propagation identification results compared against those of the transfer entropy-based monitoring method. The results show that the novel networked process monitoring and diagnosis approach can accurately detect abnormal events, identify the fault propagation pathways, and diagnose the root cause variables. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
A novel networked process monitoring, fault propagation identification, and root cause diagnosis approach is developed in this study. First, process network structure is determined from prior process knowledge and analysis. The network model parameters including the conditional probability density functions of different nodes are then estimated from process operating data to characterize the causal relationships among the monitored variables. Subsequently, the Bayesian inference-based abnormality likelihood index is proposed to detect abnormal events in chemical processes. After the process fault is detected, the novel dynamic Bayesian probability and contribution indices are further developed from the transitional probabilities of monitored variables to identify the major faulty effect variables with significant upsets. With the dynamic Bayesian contribution index, the statistical inference rules are, thus, designed to search for the fault propagation pathways from the downstream backwards to the upstream process. In this way, the ending nodes in the identified propagation pathways can be captured as the root cause variables of process faults. Meanwhile, the identified fault propagation sequence provides an in-depth understanding as to the interactive effects of faults throughout the processes. The proposed approach is demonstrated using the illustrative continuous stirred tank reactor system and the Tennessee Eastman chemical process with the fault propagation identification results compared against those of the transfer entropy-based monitoring method. The results show that the novel networked process monitoring and diagnosis approach can accurately detect abnormal events, identify the fault propagation pathways, and diagnose the root cause variables. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13958" xmlns="http://purl.org/rss/1.0/"><title>Hypoxia and flow perfusion modulate proliferation and gene expression of articular chondrocytes on porous scaffolds</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13958</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Hypoxia and flow perfusion modulate proliferation and gene expression of articular chondrocytes on porous scaffolds</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Rebecca L. Dahlin, Ville V. Meretoja, Mengwei Ni, F. Kurtis Kasper, Antonios G. Mikos</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-18T18:13:17.821512-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13958</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13958</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13958</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. Biomolecular Engineering, Bioengineering, Biochemicals, Biofuels, and Food</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The combination of reduced oxygen tension and flow perfusion bioreactor culture is investigated for its effect on the proliferation, glycosaminoglycan production, and chondrogenic gene expression of bovine articular chondrocytes on porous polymer scaffolds. It was hypothesized that the combination of such factors would more closely replicate the <em>in situ</em> environment of these cells, leading to improvements in the cell phenotype. Chondrocytes were seeded onto electrospun poly(ε-caprolactone) scaffolds and cultured in static or perfusion culture in either normoxic or hypoxic conditions for 6days. Results demonstrated that the combination of hypoxic and perfusion culture led to an increase in chondrocyte proliferation and glycosaminoglycan production, as well as an improvement in the ratio of collagen II/I gene expression over perfusion culture alone. The results demonstrate the need to combine multiple signals <em>in vitro</em>, in order to improve tissue growth by more closely replicating the native environment of cells. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The combination of reduced oxygen tension and flow perfusion bioreactor culture is investigated for its effect on the proliferation, glycosaminoglycan production, and chondrogenic gene expression of bovine articular chondrocytes on porous polymer scaffolds. It was hypothesized that the combination of such factors would more closely replicate the in situ environment of these cells, leading to improvements in the cell phenotype. Chondrocytes were seeded onto electrospun poly(ε-caprolactone) scaffolds and cultured in static or perfusion culture in either normoxic or hypoxic conditions for 6days. Results demonstrated that the combination of hypoxic and perfusion culture led to an increase in chondrocyte proliferation and glycosaminoglycan production, as well as an improvement in the ratio of collagen II/I gene expression over perfusion culture alone. The results demonstrate the need to combine multiple signals in vitro, in order to improve tissue growth by more closely replicating the native environment of cells. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14006" xmlns="http://purl.org/rss/1.0/"><title>Classification of the Degradation of Soft Sensor Models and Discussion on Adaptive Models</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14006</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Classification of the Degradation of Soft Sensor Models and Discussion on Adaptive Models</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hiromasa Kaneko, Kimito Funatsu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-14T11:03:20.387575-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14006</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14006</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14006</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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Soft sensors are used widely to estimate a process variable which is difficult to measure online. One of the crucial difficulties of soft sensors is that predictive accuracy drops due to changes of state of chemical plants. It is called as the degradation of soft sensor models. In this study, we attempted to classify this degradation of models in terms of changes in an explanatory variable and an objective variable, and the rapidity of the changes. Moreover, we discussed characteristics of adaptive soft sensor models, based on the classification results. By analyzing simulated data sets and a real industrial data set, we could obtain knowledge and information on appropriate adaptive models for each type of the degradation. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
Soft sensors are used widely to estimate a process variable which is difficult to measure online. One of the crucial difficulties of soft sensors is that predictive accuracy drops due to changes of state of chemical plants. It is called as the degradation of soft sensor models. In this study, we attempted to classify this degradation of models in terms of changes in an explanatory variable and an objective variable, and the rapidity of the changes. Moreover, we discussed characteristics of adaptive soft sensor models, based on the classification results. By analyzing simulated data sets and a real industrial data set, we could obtain knowledge and information on appropriate adaptive models for each type of the degradation. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14004" xmlns="http://purl.org/rss/1.0/"><title>Experimental and Simulation on Enantioselective Extraction in Centrifugal Contactor Separators</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14004</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Experimental and Simulation on Enantioselective Extraction in Centrifugal Contactor Separators</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Kewen Tang, Hui Zhang, Yongbing Liu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-14T10:27:41.56109-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14004</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14004</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14004</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separations: Materials, Devices and 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The increasing demand for optically pure compounds stimulates the development of new chiral separation processes on an industrial scale. The enantioselective liquid–liquid extraction (ELLE) of phenylsuccinic acid (PSA) enantiomers using hydrophilic hydroxyphenyl-β-CD as extractant (C) was studied experimentally in a countercurrent cascade of 10 centrifugal contactor separators at 293 K. Based on a single-stage equilibrium model and the law of conservation of mass, a multistage equilibrium model of ELLE was developed to investigate the influence of changes in the process parameterssuch as phase ratios and concentrations on extraction efficiency. The multistage equilibrium model was verified experimentally with a good agreement. The model was applied to predict the symmetrical separation of PSA enantiomers. By modeling, optimal process parameters for the symmetrical separation of PSA enantiomers can beachieved. The minimum number of stages was determined at 22 and 24 for ee<sub>eq</sub>&gt;98% and ee<sub>eq</sub>&gt;99%, respectively. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The increasing demand for optically pure compounds stimulates the development of new chiral separation processes on an industrial scale. The enantioselective liquid–liquid extraction (ELLE) of phenylsuccinic acid (PSA) enantiomers using hydrophilic hydroxyphenyl-β-CD as extractant (C) was studied experimentally in a countercurrent cascade of 10 centrifugal contactor separators at 293 K. Based on a single-stage equilibrium model and the law of conservation of mass, a multistage equilibrium model of ELLE was developed to investigate the influence of changes in the process parameterssuch as phase ratios and concentrations on extraction efficiency. The multistage equilibrium model was verified experimentally with a good agreement. The model was applied to predict the symmetrical separation of PSA enantiomers. By modeling, optimal process parameters for the symmetrical separation of PSA enantiomers can beachieved. The minimum number of stages was determined at 22 and 24 for eeeq&gt;98% and eeeq&gt;99%, respectively. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13998" xmlns="http://purl.org/rss/1.0/"><title>Hydrogenation of dimethyl oxalate to ethylene glycol over mesoporous Cu-MCM-41 catalysts</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13998</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Hydrogenation of dimethyl oxalate to ethylene glycol over mesoporous Cu-MCM-41 catalysts</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Xinbin Ma, Hanwen Chi, Hairong Yue, Yujun Zhao, Yan Xu, Jing Lv, Shengping Wang, Jinlong Gong</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-11T16:22:10.347968-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13998</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13998</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13998</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, 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[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The synthesis and utilization of mesoporous <span class="fixed-roman">Cu</span>-MCM-41 catalysts for hydrogenation of dimethyl oxalate to ethylene glycol is described in this article. Physicochemical properties of these <span class="fixed-roman">Cu</span>-MCM-41 catalysts have been investigated by <span class="fixed-roman">N</span><sub>2</sub>-physisorption, X-ray diffraction, inductively coupled plasma, <span class="fixed-roman">N</span><sub>2</sub><span class="fixed-roman">O</span> titration, transmission electron microscopy, temperature programmed reduction, Fourier transform infrared spectroscopy, and X-ray photoelectron spectroscopy. It was found that the copper loading significantly influenced the pore structure and copper surface area of the catalyst. High catalytic performance is obtained over a 20<span class="fixed-roman">Cu</span>-MCM-41 catalyst with a full DMO conversion and EG yield of 92% at a LHSV of 3.0 h<sup>−1</sup>. The catalytic performance of optimized 20<span class="fixed-roman">Cu</span>-MCM-41 catalyst could be attributed to the fine copper dispersion and large copper surface areas. © 2013 American Institute of Chemical Engineers <em>AIChE J</em>, 2013</p></div>
]]></content:encoded><description>
The synthesis and utilization of mesoporous Cu-MCM-41 catalysts for hydrogenation of dimethyl oxalate to ethylene glycol is described in this article. Physicochemical properties of these Cu-MCM-41 catalysts have been investigated by N2-physisorption, X-ray diffraction, inductively coupled plasma, N2O titration, transmission electron microscopy, temperature programmed reduction, Fourier transform infrared spectroscopy, and X-ray photoelectron spectroscopy. It was found that the copper loading significantly influenced the pore structure and copper surface area of the catalyst. High catalytic performance is obtained over a 20Cu-MCM-41 catalyst with a full DMO conversion and EG yield of 92% at a LHSV of 3.0 h−1. The catalytic performance of optimized 20Cu-MCM-41 catalyst could be attributed to the fine copper dispersion and large copper surface areas. © 2013 American Institute of Chemical Engineers AIChE J, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13965" xmlns="http://purl.org/rss/1.0/"><title>The stability of direct carbon fuel cells with molten Sb and Sb–Bi alloy anodes</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13965</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">The stability of direct carbon fuel cells with molten Sb and Sb–Bi alloy anodes</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Abhimanyu Jayakumar, Ashay Javadekar, Jacob Gissinger, John M. Vohs, George W. Huber, Raymond J. Gorte</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-11-26T12:22:26.30257-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13965</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13965</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13965</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Tribute to Founders: Neal R. Amundson. Reaction Engineering, 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>The long-term stability of direct carbon fuel cells, based on solid oxide fuel cells with molten Sb and Sb–Bi anodes, was examined for operation with activated charcoal, rice starch, and bio-oil fuels at 973 K. With intermittent stirring of the fuel–metal anode interface, the anode performance was stable, and reasonable power densities (∼250 mW/cm<sup>2</sup>) were achieved for periods up to 250 h. With Sc-stabilized zirconia, severe thinning of the electrolyte occurred in regions of high current flow. No electrolyte thinning was observed with yttria-stabilized zirconia as the electrolyte operating at the same current densities. © 2012 American Institute of Chemical Engineers AIChE J, 2012</p></div>
]]></content:encoded><description>

The long-term stability of direct carbon fuel cells, based on solid oxide fuel cells with molten Sb and Sb–Bi anodes, was examined for operation with activated charcoal, rice starch, and bio-oil fuels at 973 K. With intermittent stirring of the fuel–metal anode interface, the anode performance was stable, and reasonable power densities (∼250 mW/cm2) were achieved for periods up to 250 h. With Sc-stabilized zirconia, severe thinning of the electrolyte occurred in regions of high current flow. No electrolyte thinning was observed with yttria-stabilized zirconia as the electrolyte operating at the same current densities. © 2012 American Institute of Chemical Engineers AIChE J, 2012
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.11232" xmlns="http://purl.org/rss/1.0/"><title>Flow structure and particle motions in a gas-polyethylene fluidized bed</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.11232</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Flow structure and particle motions in a gas-polyethylene fluidized bed</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">X. Fan, Z. Yang, D. J. Parker</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2007-06-14T00:00:00-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.11232</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.11232</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.11232</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Particle Technology and Fluidization</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="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>It has come to the attention of the editor and publisher that this article was submitted and published online on June 14, 2007 without the knowledge of one of the authors who was removed from the author list.</p></div><div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The <em>AIChE Journal</em> retracts the paper and apologize to our readership.</p></div>]]></content:encoded><description>It has come to the attention of the editor and publisher that this article was submitted and published online on June 14, 2007 without the knowledge of one of the authors who was removed from the author list.The AIChE Journal retracts the paper and apologize to our readership.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14123" xmlns="http://purl.org/rss/1.0/"><title>Celebrating singularities: Mathematics and chemical engineering</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14123</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Celebrating singularities: Mathematics and chemical engineering</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yunshan Wang, Xinguang Cheng, Hsueh-Chia Chang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-08T08:55:35.931981-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14123</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14123</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14123</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Journal Review: Transport Phenomena and Fluid Mechanics</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1830</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1843</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The authors review and project their group's work in reaction engineering, electrokinetics, thin-film lubrication/wetting, biosensing, mass spectrometry, etc., that share one common mathematical underpinning: singularities. These can be geometric singularities of actual surfaces or objects, where focused electrical, acoustic, optical and shear-stress fields produce anomalous physical phenomena that have been explored mathematically with a spectral theory or exploited for specific applications. They are also singularities of mathematical manifolds, such as solution branches and Riemann manifolds, defined by abstract mathematical formulations, so that they can be used to design optical sensors, and understand nonlinear dynamical behavior that is relevant to system control and surface characterization. The common mathematical framework for these diverse topics underscores how mathematics can reveal, organize and inspire real and industrially relevant problems in chemical engineering. © 2013 American Institute of Chemical Engineers AIChE J, 59: 1830–1843, 2013</p></div>
]]></content:encoded><description>
The authors review and project their group's work in reaction engineering, electrokinetics, thin-film lubrication/wetting, biosensing, mass spectrometry, etc., that share one common mathematical underpinning: singularities. These can be geometric singularities of actual surfaces or objects, where focused electrical, acoustic, optical and shear-stress fields produce anomalous physical phenomena that have been explored mathematically with a spectral theory or exploited for specific applications. They are also singularities of mathematical manifolds, such as solution branches and Riemann manifolds, defined by abstract mathematical formulations, so that they can be used to design optical sensors, and understand nonlinear dynamical behavior that is relevant to system control and surface characterization. The common mathematical framework for these diverse topics underscores how mathematics can reveal, organize and inspire real and industrially relevant problems in chemical engineering. © 2013 American Institute of Chemical Engineers AIChE J, 59: 1830–1843, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13988" xmlns="http://purl.org/rss/1.0/"><title>Modeling, Simulation, and Optimization of Hybrid Fe(II)/Fe(III) Redox Flow Fuel Cell System</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13988</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Modeling, Simulation, and Optimization of Hybrid Fe(II)/Fe(III) Redox Flow Fuel Cell System</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hossein Hojjati, Kalin Penev, Victor R. Pupkevich, Dimitre G. Karamanev</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-20T13:58:17.728446-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13988</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13988</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13988</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Biomolecular Engineering, Bioengineering, Biochemicals, Biofuels, and Food</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1844</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1854</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The kinetic parameters of ferrous iron oxidation, covering both lag and growth phases at low pH, were determined using a free suspended culture of the bacterium Leptospirillum ferriphilum. A mathematical model was developed to simulate the dynamics of a continuous bioreactor used for operation of a novel hybrid Fe(II)/Fe(III) redox flow fuel cell system. By changing the current load within a predefined range, three runs were performed to predict time-varying ferrous iron concentration, bacterial cell concentration, and pH as the major output variables of simulation program. The model was experimentally validated through three runs. It was found out that the key variable in dynamic analysis of the bioreactor was the current load applied. To optimize the bioreactor and the fuel cell conditions for a normal-steady-state operation, the optimal current profile for a transient phase was determined. A selected optimal policy was also implemented and validated during the mini-pilot-scale system experiments. © 2013 American Institute of Chemical Engineers AIChE J, 59: 1844–1854, 2013</p></div>
]]></content:encoded><description>
The kinetic parameters of ferrous iron oxidation, covering both lag and growth phases at low pH, were determined using a free suspended culture of the bacterium Leptospirillum ferriphilum. A mathematical model was developed to simulate the dynamics of a continuous bioreactor used for operation of a novel hybrid Fe(II)/Fe(III) redox flow fuel cell system. By changing the current load within a predefined range, three runs were performed to predict time-varying ferrous iron concentration, bacterial cell concentration, and pH as the major output variables of simulation program. The model was experimentally validated through three runs. It was found out that the key variable in dynamic analysis of the bioreactor was the current load applied. To optimize the bioreactor and the fuel cell conditions for a normal-steady-state operation, the optimal current profile for a transient phase was determined. A selected optimal policy was also implemented and validated during the mini-pilot-scale system experiments. © 2013 American Institute of Chemical Engineers AIChE J, 59: 1844–1854, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13963" xmlns="http://purl.org/rss/1.0/"><title>A practical approach to produce Mg-Al spinel based on the modeling of phase equilibria for NH4Cl-MgCl2-AlCl3-H2O system</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13963</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A practical approach to produce Mg-Al spinel based on the modeling of phase equilibria for NH4Cl-MgCl2-AlCl3-H2O system</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Wencheng Gao, Zhibao Li</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-11-30T08:59:02.996873-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13963</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13963</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13963</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Inorganic Materials: Synthesis and Processing</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1855</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1867</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Based on chemical modeling of phase equilibria for the NH<sub>4</sub>Cl-MgCl<sub>2</sub>-AlCl<sub>3</sub>-H<sub>2</sub>O system, a practical approach to produce Mg-Al spinel (MgAl<sub>2</sub>O<sub>4</sub>) (widely used as refractory brick, supports in catalysts, and inert material for oxygen carriers) is proposed and proven feasible. This novel process includes coprecipitation of Mg<sub>4</sub>Al<sub>2</sub>(OH)<sub>14</sub>·3H<sub>2</sub>O from the NH<sub>3</sub>-MgCl<sub>2</sub>-AlCl<sub>3</sub>-H<sub>2</sub>O system; calcination of Mg<sub>4</sub>Al<sub>2</sub>(OH)<sub>14</sub>·3H<sub>2</sub>O to obtain Mg-Al spinel and recovery of NH<sub>4</sub>Cl from NH<sub>4</sub>Cl-rich solutions by feeding MgCl<sub>2</sub>-AlCl<sub>3</sub>. A MSMPR reactor was applied to investigate the effect of temperature, feed concentration, and NH<sub>4</sub>Cl addition on coprecipitation of precursor Mg<sub>4</sub>Al<sub>2</sub>(OH)<sub>14</sub>·3H<sub>2</sub>O from MgCl<sub>2</sub>-AlCl<sub>3</sub> solutions with Mg/Al ratio = 2 through gradual addition of NH<sub>4</sub>OH. The phase equilibria of the NH<sub>4</sub>Cl-MgCl<sub>2</sub>-AlCl<sub>3</sub>-H<sub>2</sub>O system were determined over the temperature range 283.2 to 363.2 K using dynamic method. The experimental solubilities were regressed to obtain new Bromley-Zemaitis model parameters. These newly obtained parameters were verified by predicting the quaternary system. A chemical model for the NH<sub>4</sub>Cl-MgCl<sub>2</sub>-AlCl<sub>3</sub>-H<sub>2</sub>O system has been established with the OLI platform. All the results generated from this study will provide the theoretical basis for Mg-Al spinel production. The high quality Mg-Al spinel was prepared by calcination of precursor from 773.2 to 1273.2 K, and the NH<sub>4</sub>Cl was successfully recovered through the common ion effect of MgCl<sub>2</sub>-AlCl<sub>3</sub> addition. © 2012 American Institute of Chemical Engineers AIChE J, 59: 1855–1867, 2013</p></div>
]]></content:encoded><description>
Based on chemical modeling of phase equilibria for the NH4Cl-MgCl2-AlCl3-H2O system, a practical approach to produce Mg-Al spinel (MgAl2O4) (widely used as refractory brick, supports in catalysts, and inert material for oxygen carriers) is proposed and proven feasible. This novel process includes coprecipitation of Mg4Al2(OH)14·3H2O from the NH3-MgCl2-AlCl3-H2O system; calcination of Mg4Al2(OH)14·3H2O to obtain Mg-Al spinel and recovery of NH4Cl from NH4Cl-rich solutions by feeding MgCl2-AlCl3. A MSMPR reactor was applied to investigate the effect of temperature, feed concentration, and NH4Cl addition on coprecipitation of precursor Mg4Al2(OH)14·3H2O from MgCl2-AlCl3 solutions with Mg/Al ratio = 2 through gradual addition of NH4OH. The phase equilibria of the NH4Cl-MgCl2-AlCl3-H2O system were determined over the temperature range 283.2 to 363.2 K using dynamic method. The experimental solubilities were regressed to obtain new Bromley-Zemaitis model parameters. These newly obtained parameters were verified by predicting the quaternary system. A chemical model for the NH4Cl-MgCl2-AlCl3-H2O system has been established with the OLI platform. All the results generated from this study will provide the theoretical basis for Mg-Al spinel production. The high quality Mg-Al spinel was prepared by calcination of precursor from 773.2 to 1273.2 K, and the NH4Cl was successfully recovered through the common ion effect of MgCl2-AlCl3 addition. © 2012 American Institute of Chemical Engineers AIChE J, 59: 1855–1867, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13968" xmlns="http://purl.org/rss/1.0/"><title>The Influence of Process Parameters on the Properties of PLGA-Microparticles Produced by the Emulsion Extraction Method</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13968</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">The Influence of Process Parameters on the Properties of PLGA-Microparticles Produced by the Emulsion Extraction Method</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Nikolett Kiss, Günter Brenn, Daniele Suzzi, Stefan Scheler, Herwig Jennewein, Juliana Wieser, Johannes Khinast</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-20T10:44:55.389848-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13968</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13968</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13968</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Particle Technology and Fluidization</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1868</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1881</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Controlled release poly(lactic-co-glycolic acid) microparticles for use as active pharmaceutical ingredient carriers were prepared by the emulsion extraction method. Particle formation experiments were carried out in a stirred vessel. The local flow conditions in these experiments, that is, local shear rates and dissipation rates, and the extraction rate of the organic solvent were examined by a computational fluid dynamics (CFD) simulation. The local flow conditions in the stirred tank reactor have a significant influence on the final properties, specific surface area, skeletal density, organic solvent content, and size of the microparticles. We determined nondimensional correlations for predicting these particle properties as functions of the process parameters as, for example, the stirrer speed, emulsion injection point, and oil droplet size in the initial emulsion. The results demonstrate that CFD simulations offer insight into the particle formation process for different batch sizes and provide a basis for scale-up and optimization of the process. © 2012 American Institute of Chemical Engineers AIChE J, 59: 1868–1881, 2013</p></div>
]]></content:encoded><description>
Controlled release poly(lactic-co-glycolic acid) microparticles for use as active pharmaceutical ingredient carriers were prepared by the emulsion extraction method. Particle formation experiments were carried out in a stirred vessel. The local flow conditions in these experiments, that is, local shear rates and dissipation rates, and the extraction rate of the organic solvent were examined by a computational fluid dynamics (CFD) simulation. The local flow conditions in the stirred tank reactor have a significant influence on the final properties, specific surface area, skeletal density, organic solvent content, and size of the microparticles. We determined nondimensional correlations for predicting these particle properties as functions of the process parameters as, for example, the stirrer speed, emulsion injection point, and oil droplet size in the initial emulsion. The results demonstrate that CFD simulations offer insight into the particle formation process for different batch sizes and provide a basis for scale-up and optimization of the process. © 2012 American Institute of Chemical Engineers AIChE J, 59: 1868–1881, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13974" xmlns="http://purl.org/rss/1.0/"><title>Bubble formation in an annular granular jet dispersed by a central air round jet</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13974</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Bubble formation in an annular granular jet dispersed by a central air round jet</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hui Lu, Hai-Feng Liu, Wei-Feng Li, Jian-Liang Xu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-26T12:48:12.950648-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13974</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13974</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13974</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Particle Technology and Fluidization</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1882</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1893</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>An annular granular jet surrounding an air jet at its core is studied experimentally using high-speed digital photography. The experimental results show that particle bubbles in a periodic manner are formed whether the central air is swirling or not. This flow feature is induced by the intense interaction between the central air jet and the annular granular jet, and it is important for the dispersion of particles by the air jet in the near field. The interaction between the two phases is mainly intensified by higher superficial air jet velocity and the addition of swirl to the central air jet. The bubbling frequency, bubble size, bubble shape, and bubble growth rate are investigated by analyzing a large number of images. In addition, the dispersion angle of granular jet is found to be mainly governed by the radial growth rate of the bubble. © 2012 American Institute of Chemical Engineers AIChE J, 59: 1882–1893, 2013</p></div>
]]></content:encoded><description>
An annular granular jet surrounding an air jet at its core is studied experimentally using high-speed digital photography. The experimental results show that particle bubbles in a periodic manner are formed whether the central air is swirling or not. This flow feature is induced by the intense interaction between the central air jet and the annular granular jet, and it is important for the dispersion of particles by the air jet in the near field. The interaction between the two phases is mainly intensified by higher superficial air jet velocity and the addition of swirl to the central air jet. The bubbling frequency, bubble size, bubble shape, and bubble growth rate are investigated by analyzing a large number of images. In addition, the dispersion angle of granular jet is found to be mainly governed by the radial growth rate of the bubble. © 2012 American Institute of Chemical Engineers AIChE J, 59: 1882–1893, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13982" xmlns="http://purl.org/rss/1.0/"><title>Characterization of Mixing and Size Segregation in a Rotating Drum by a Particle Tracking Method</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13982</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Characterization of Mixing and Size Segregation in a Rotating Drum by a Particle Tracking Method</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ebrahim Alizadeh, Olivier Dubé, François Bertrand, Jamal Chaouki</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-04T04:30:11.521567-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13982</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13982</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13982</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Particle Technology and Fluidization</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1894</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1905</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The mechanisms of segregation in solids mixing, even in simple rotating drums, are not clearly understood. Although most past studies have focused on binary mixtures, this work investigates the effect of polydispersity on granular flow, mixing, and segregation in a rotating drum operated in rolling regime through particle trajectories obtained from the radioactive particle tracking technique. Velocity profiles, radial segregation, and axial dispersion coefficients for monodisperse and polydisperse systems of glass beads are analyzed with respect to rotational speed and particle size. A model is introduced to predict the residence times along streamlines and evaluate the rate at which the material renews at the free surface and within the inner layers of the bed. Our results reveal similar velocity profiles and residence times for monodisperse and polydisperse systems. They also indicate that the particles distribute along the radial direction of the drum, although not necessarily in a core/shell configuration. © 2012 American Institute of Chemical Engineers AIChE J, 59: 1894–1905, 2013</p></div>
]]></content:encoded><description>
The mechanisms of segregation in solids mixing, even in simple rotating drums, are not clearly understood. Although most past studies have focused on binary mixtures, this work investigates the effect of polydispersity on granular flow, mixing, and segregation in a rotating drum operated in rolling regime through particle trajectories obtained from the radioactive particle tracking technique. Velocity profiles, radial segregation, and axial dispersion coefficients for monodisperse and polydisperse systems of glass beads are analyzed with respect to rotational speed and particle size. A model is introduced to predict the residence times along streamlines and evaluate the rate at which the material renews at the free surface and within the inner layers of the bed. Our results reveal similar velocity profiles and residence times for monodisperse and polydisperse systems. They also indicate that the particles distribute along the radial direction of the drum, although not necessarily in a core/shell configuration. © 2012 American Institute of Chemical Engineers AIChE J, 59: 1894–1905, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13999" xmlns="http://purl.org/rss/1.0/"><title>Numerical study of mixing and thermal conduction of granular particles in rotating tumblers</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13999</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Numerical study of mixing and thermal conduction of granular particles in rotating tumblers</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Nan Gui, Jinsen Gao, Zhongli Ji</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-24T09:17:10.914339-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13999</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13999</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13999</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Particle Technology and Fluidization</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1906</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1918</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A discrete element method (DEM) study is conducted to investigate the mixing and heat-transfer characteristics of steel spherical particles under various rotation speeds and flow regimes of a rotating tumbler. The mixing degree, weighted temperature, temperature discrepancy at the mixing interface, temperature radial distribution, and information entropy are used to analyze the effect of mixing structure and evolution duration on the heat-transfer characteristics. The results under the same revolution and the same evolution time are compared to show the effects of evolution time and mixing structure on thermal conduction. After a detailed analysis, the joint contribution of mixing degree and duration to granular heat transfer is explained, and the different approaches in static thermal conduction and dynamic mixing are shown. Moreover, a new method is proposed using the mean increase rate of temperature information entropy to determine the most effective operating condition for thermal conduction in granular particles. © 2013 American Institute of Chemical Engineers AIChE J, 59: 1906–1918, 2013</p></div>
]]></content:encoded><description>
A discrete element method (DEM) study is conducted to investigate the mixing and heat-transfer characteristics of steel spherical particles under various rotation speeds and flow regimes of a rotating tumbler. The mixing degree, weighted temperature, temperature discrepancy at the mixing interface, temperature radial distribution, and information entropy are used to analyze the effect of mixing structure and evolution duration on the heat-transfer characteristics. The results under the same revolution and the same evolution time are compared to show the effects of evolution time and mixing structure on thermal conduction. After a detailed analysis, the joint contribution of mixing degree and duration to granular heat transfer is explained, and the different approaches in static thermal conduction and dynamic mixing are shown. Moreover, a new method is proposed using the mean increase rate of temperature information entropy to determine the most effective operating condition for thermal conduction in granular particles. © 2013 American Institute of Chemical Engineers AIChE J, 59: 1906–1918, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13990" xmlns="http://purl.org/rss/1.0/"><title>Pilot-scale investigation and CFD modeling of particle deposition in low-dust monolithic SCR DeNOx catalysts</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13990</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Pilot-scale investigation and CFD modeling of particle deposition in low-dust monolithic SCR DeNOx catalysts</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Michael Lykke Heiredal, Anker Degn Jensen, Joakim Reimer Thøgersen, Flemming Jappe Frandsen, Jens-Uwe Friemann</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-31T13:21:52.807494-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13990</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13990</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13990</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Particle Technology and Fluidization</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1919</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1933</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Deposition of particles in selective catalytic reduction DeNO<sub>x</sub> monolithic catalysts was studied by low-dust pilot-scale experiments. The experiments showed a total deposition efficiency of about 30%, and the deposition pattern was similar to that observed in full-scale low-dust applications. On extended exposure to the dust-laden flue gas, complete blocking of channels was observed, showing that also in low-dust applications soot blowing is necessary to keep the catalyst clean. A particle deposition model was developed in computational fluid dynamics, and simulations were carried out assuming either laminar or turbulent flow. Assuming laminar flow, the accumulated mass was underpredicted with a factor of about 17, whereas assuming turbulent flow overpredicted the experimental result with a factor of about 2. The simulations showed that turbulent diffusion in the monolith channels and inertial impaction and gravitational settling on the top of the monolith were the dominating mechanisms for particle deposition on the catalyst. © 2013 American Institute of Chemical Engineers AIChE J, 59: 1919–1933, 2013</p></div>
]]></content:encoded><description>
Deposition of particles in selective catalytic reduction DeNOx monolithic catalysts was studied by low-dust pilot-scale experiments. The experiments showed a total deposition efficiency of about 30%, and the deposition pattern was similar to that observed in full-scale low-dust applications. On extended exposure to the dust-laden flue gas, complete blocking of channels was observed, showing that also in low-dust applications soot blowing is necessary to keep the catalyst clean. A particle deposition model was developed in computational fluid dynamics, and simulations were carried out assuming either laminar or turbulent flow. Assuming laminar flow, the accumulated mass was underpredicted with a factor of about 17, whereas assuming turbulent flow overpredicted the experimental result with a factor of about 2. The simulations showed that turbulent diffusion in the monolith channels and inertial impaction and gravitational settling on the top of the monolith were the dominating mechanisms for particle deposition on the catalyst. © 2013 American Institute of Chemical Engineers AIChE J, 59: 1919–1933, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13980" xmlns="http://purl.org/rss/1.0/"><title>3-D numerical simulations on flow and mixing behaviors in gas–liquid–solid microchannels</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13980</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">3-D numerical simulations on flow and mixing behaviors in gas–liquid–solid microchannels</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Tang Can, Liu Mingyan, Xu Yonggui</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-07T16:37:22.089693-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13980</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13980</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13980</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Particle Technology and Fluidization</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1934</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1951</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Three-dimensional (3-D) gas-liquid–solid flow and mixing behaviors in microchannels were simulated by coupled volume of fluid and discrete phase method and simulations were validated against observations. The detachment time and length of gas slug are shortened in liquid–solid flow, compared with those in liquid flow due to higher superficial viscosity of liquid–solid mixture, which will move the bubble formation toward the dripping regime. Solid particles mainly distribute in liquid slug and particle flow shows obvious periodicity. With the increase of contact angle of the inner wall, gas slug (0–50°), stratified (77–120°), and liquid drop (160°) flows are observed. The residence time distributions of solid and liquid phases are similar because particles behave as tracers. The backmixing of solid and liquid phases in liquid drop flow is the weakest among the three flow patterns, and the backmixing of gas phase in slug flow is weaker than that in both stratified and liquid drop flows. The results can provide a theoretical basis for the design of microreactors. © 2013 American Institute of Chemical Engineers AIChE J, 59: 1934–1951, 2013</p></div>
]]></content:encoded><description>
Three-dimensional (3-D) gas-liquid–solid flow and mixing behaviors in microchannels were simulated by coupled volume of fluid and discrete phase method and simulations were validated against observations. The detachment time and length of gas slug are shortened in liquid–solid flow, compared with those in liquid flow due to higher superficial viscosity of liquid–solid mixture, which will move the bubble formation toward the dripping regime. Solid particles mainly distribute in liquid slug and particle flow shows obvious periodicity. With the increase of contact angle of the inner wall, gas slug (0–50°), stratified (77–120°), and liquid drop (160°) flows are observed. The residence time distributions of solid and liquid phases are similar because particles behave as tracers. The backmixing of solid and liquid phases in liquid drop flow is the weakest among the three flow patterns, and the backmixing of gas phase in slug flow is weaker than that in both stratified and liquid drop flows. The results can provide a theoretical basis for the design of microreactors. © 2013 American Institute of Chemical Engineers AIChE J, 59: 1934–1951, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13997" xmlns="http://purl.org/rss/1.0/"><title>Multifluid Modeling of the Desulfurization Process within a Bubbling Fluidized Bed Coal Gasifier</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13997</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Multifluid Modeling of the Desulfurization Process within a Bubbling Fluidized Bed Coal Gasifier</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Lindsay-Marie Armstrong, Sai Gu, Kai H. Luo, Pinakeswar Mahanta</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-25T20:51:48.76987-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13997</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13997</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13997</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Particle Technology and Fluidization</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1952</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1963</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The desulfurization process to a two-dimensional (2-D) and three-dimensional (3-D) Eulerian–Eulerian computational fluid dynamic (CFD) model of a coal bubbling fluidized gasifier is introduced. The desulfurization process is important for the reduction of harmful SO<sub>x</sub> emissions; therefore, the development of a CFD model capable of predicting chemical reactions involving desulfurization is key to the optimization of reactor designs and operating conditions. To model the process, one gaseous phase and five particulate phases are included. Devolatilization, heterogeneous, and homogeneous chemical reactions as well as calcination and desulfurization reactions are incorporated. A calcination-only model and a calcination plus desulfurization model are simulated in 2-D and 3-D and the concentrations of SO<sub>2</sub> leaving the reactors are compared. The simulated results are assessed against available published experimental data. The influence of the fluidized bed on the desulfurization is also considered. © 2013 American Institute of Chemical Engineers AIChE J, 59: 1952–1963, 2013</p></div>
]]></content:encoded><description>
The desulfurization process to a two-dimensional (2-D) and three-dimensional (3-D) Eulerian–Eulerian computational fluid dynamic (CFD) model of a coal bubbling fluidized gasifier is introduced. The desulfurization process is important for the reduction of harmful SOx emissions; therefore, the development of a CFD model capable of predicting chemical reactions involving desulfurization is key to the optimization of reactor designs and operating conditions. To model the process, one gaseous phase and five particulate phases are included. Devolatilization, heterogeneous, and homogeneous chemical reactions as well as calcination and desulfurization reactions are incorporated. A calcination-only model and a calcination plus desulfurization model are simulated in 2-D and 3-D and the concentrations of SO2 leaving the reactors are compared. The simulated results are assessed against available published experimental data. The influence of the fluidized bed on the desulfurization is also considered. © 2013 American Institute of Chemical Engineers AIChE J, 59: 1952–1963, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13962" xmlns="http://purl.org/rss/1.0/"><title>Novel method for targeting the optimal purification feed flow rate of hydrogen network with purification reuse/recycle</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13962</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Novel method for targeting the optimal purification feed flow rate of hydrogen network with purification reuse/recycle</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Guilian Liu, Hao Li, Xiao Feng, Chun Deng</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-11-30T08:59:46.161123-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13962</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13962</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13962</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/">1964</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1980</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The purification reuse/recycle is one effective resource conservation strategy. In this article, a novel conceptual method is proposed to identify the optimal purification feed flow rate (PFFR) and the corresponding maximum hydrogen utility savings (HUS) of the hydrogen network with purification reuse/recycle. In this method, the sources and sink-tie-lines are divided into three regions according to the purified product and purification feed. The quantitative relationship between the HUS and the PFFR is analyzed for the sink-tie-lines and sources of each region. With the quantitative relationship line between the HUS and the PFFR of each source plotted, the quantitative relationship diagram can be obtained and can be used to identify the pinch point and the HUS for a given PFFR. Furthermore, the optimal PFFR and the maximum HUS can be identified easily. Three cases are studied to illustrate the applicability of the proposed method. © 2012 American Institute of Chemical Engineers AIChE J, 59: 1964–1980, 2013</p></div>
]]></content:encoded><description>
The purification reuse/recycle is one effective resource conservation strategy. In this article, a novel conceptual method is proposed to identify the optimal purification feed flow rate (PFFR) and the corresponding maximum hydrogen utility savings (HUS) of the hydrogen network with purification reuse/recycle. In this method, the sources and sink-tie-lines are divided into three regions according to the purified product and purification feed. The quantitative relationship between the HUS and the PFFR is analyzed for the sink-tie-lines and sources of each region. With the quantitative relationship line between the HUS and the PFFR of each source plotted, the quantitative relationship diagram can be obtained and can be used to identify the pinch point and the HUS for a given PFFR. Furthermore, the optimal PFFR and the maximum HUS can be identified easily. Three cases are studied to illustrate the applicability of the proposed method. © 2012 American Institute of Chemical Engineers AIChE J, 59: 1964–1980, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13957" xmlns="http://purl.org/rss/1.0/"><title>Experimental evaluation of an approach to online redesign of experiments for parameter determination</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13957</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Experimental evaluation of an approach to online redesign of experiments for parameter determination</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Tilman Barz, Diana C. López Cárdenas, Harvey Arellano-Garcia, Günter Wozny</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-03T11:07:48.042273-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13957</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13957</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13957</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/">1981</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1995</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The online redesign of experiments for parameter determination of nonlinear dynamic systems has been studied recently by different research groups. In this article, this technique is assessed in a real case study for the first time. The presented algorithm adopts well-known concepts from model-based control. Compared to previous studies, special attention is given to the efficient treatment of the underlying nonlinear and possibly ill-conditioned parameter estimation and experiment design problems. These problems are solved with single shooting and gradient-based nonlinear programming (NLP) solvers. We use an initial value solver, which generates first- and second-order sensitivities to compute exact derivatives of the problem functions. As a special feature, we propose the integration of a local parameter identifiability analysis and a corresponding algorithm that generates well-conditioned problems. The practical applicability is demonstrated by experimental application to a chromatography column system where A, D, and E optimal experiments are performed. © 2012 American Institute of Chemical Engineers AIChE J, 59: 1981–1995, 2013</p></div>
]]></content:encoded><description>
The online redesign of experiments for parameter determination of nonlinear dynamic systems has been studied recently by different research groups. In this article, this technique is assessed in a real case study for the first time. The presented algorithm adopts well-known concepts from model-based control. Compared to previous studies, special attention is given to the efficient treatment of the underlying nonlinear and possibly ill-conditioned parameter estimation and experiment design problems. These problems are solved with single shooting and gradient-based nonlinear programming (NLP) solvers. We use an initial value solver, which generates first- and second-order sensitivities to compute exact derivatives of the problem functions. As a special feature, we propose the integration of a local parameter identifiability analysis and a corresponding algorithm that generates well-conditioned problems. The practical applicability is demonstrated by experimental application to a chromatography column system where A, D, and E optimal experiments are performed. © 2012 American Institute of Chemical Engineers AIChE J, 59: 1981–1995, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13964" xmlns="http://purl.org/rss/1.0/"><title>Economic plantwide control of the ethyl benzene process</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13964</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Economic plantwide control of the ethyl benzene process</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Rahul Jagtap, Ashok S Pathak, Nitin Kaistha</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-10T18:47:33.475132-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13964</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13964</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13964</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/">1996</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2014</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Systematic plantwide control system design for economically optimal operation of the ethyl benzene process over a large throughput range is studied. As throughput is increased, constraints progressively become active with the highest number of active constraints at maximum throughput. An economic plantwide control system (CS1) is designed for operation at this most constrained operating point using a novel “top-down” pairing approach with higher prioritization to the economic objectives over regulatory objectives. This structure is adapted for near optimal low throughput operation with constraints that go inactive taking up additional economic variable control. For comparison, a conventional plantwide control structure (CS2) with the throughput manipulator at a fresh feed and “bottom-up” pairing for the control objectives is also synthesized. Four overrides are needed in CS2 to handle the hard equipment capacity constraints at maximum throughput. Rigorous dynamic simulations show that CS1 is dynamically and economically significantly superior to CS2. © 2012 American Institute of Chemical Engineers AIChE J, 59: 1996–2014, 2013</p></div>
]]></content:encoded><description>
Systematic plantwide control system design for economically optimal operation of the ethyl benzene process over a large throughput range is studied. As throughput is increased, constraints progressively become active with the highest number of active constraints at maximum throughput. An economic plantwide control system (CS1) is designed for operation at this most constrained operating point using a novel “top-down” pairing approach with higher prioritization to the economic objectives over regulatory objectives. This structure is adapted for near optimal low throughput operation with constraints that go inactive taking up additional economic variable control. For comparison, a conventional plantwide control structure (CS2) with the throughput manipulator at a fresh feed and “bottom-up” pairing for the control objectives is also synthesized. Four overrides are needed in CS2 to handle the hard equipment capacity constraints at maximum throughput. Rigorous dynamic simulations show that CS1 is dynamically and economically significantly superior to CS2. © 2012 American Institute of Chemical Engineers AIChE J, 59: 1996–2014, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13975" xmlns="http://purl.org/rss/1.0/"><title>Enhancing mass and energy integration by external recycle in reactive distillation columns</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13975</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Enhancing mass and energy integration by external recycle in reactive distillation columns</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Haisheng Chen, Kejin Huang, Wei Liu, Liang Zhang, Shaofeng Wang, San-Jang Wang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-26T15:42:01.875446-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13975</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13975</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13975</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/">2015</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2032</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The synthesis and design of reactive distillation columns separating reacting mixtures with the most unfavorable relative volatilities (i.e., the reactants are the heaviest and lightest components with the products being the intermediate ones) are described. The unfavorable thermodynamics poses great difficulties in combining the reaction operation and the separation operation involved and limits severely the potential of reactive distillation columns in the reduction of capital investment (CI) and operating cost. To remove the limitation, we propose two strategies for facilitating the synthesis and design of this kind of reactive distillation columns in this article. One is to arrange prudentially the reactive section so as to strengthen internal energy integration between the reaction operation and the separation operation involved; that is, while the reactive section should be placed at the bottom of the reactive distillation columns separating exothermic reactions, it should be at the top of the reactive distillation columns separating endothermic reactions. The other is to introduce an external recycle flow between the two ends of the reactive distillation columns to reinforce internal mass integration and internal energy integration between the reaction operation and the separation operation involved; that is, whereas the external recycle flow should be directed from the top to bottom of the reactive distillation columns separating exothermic reactions, it should be from the bottom to top of the reactive distillation columns separating endothermic reactions. Separation of four hypothetical ideal (i.e., two quaternary and two ternary systems, respectively) and two real nonideal (i.e., two quaternary systems) reacting mixtures is chosen to evaluate the proposed strategies. The results show that they can considerably lower energy requirement besides a further reduction in CI. © 2012 American Institute of Chemical Engineers AIChE J, 59: 2015–2032, 2013</p></div>
]]></content:encoded><description>
The synthesis and design of reactive distillation columns separating reacting mixtures with the most unfavorable relative volatilities (i.e., the reactants are the heaviest and lightest components with the products being the intermediate ones) are described. The unfavorable thermodynamics poses great difficulties in combining the reaction operation and the separation operation involved and limits severely the potential of reactive distillation columns in the reduction of capital investment (CI) and operating cost. To remove the limitation, we propose two strategies for facilitating the synthesis and design of this kind of reactive distillation columns in this article. One is to arrange prudentially the reactive section so as to strengthen internal energy integration between the reaction operation and the separation operation involved; that is, while the reactive section should be placed at the bottom of the reactive distillation columns separating exothermic reactions, it should be at the top of the reactive distillation columns separating endothermic reactions. The other is to introduce an external recycle flow between the two ends of the reactive distillation columns to reinforce internal mass integration and internal energy integration between the reaction operation and the separation operation involved; that is, whereas the external recycle flow should be directed from the top to bottom of the reactive distillation columns separating exothermic reactions, it should be from the bottom to top of the reactive distillation columns separating endothermic reactions. Separation of four hypothetical ideal (i.e., two quaternary and two ternary systems, respectively) and two real nonideal (i.e., two quaternary systems) reacting mixtures is chosen to evaluate the proposed strategies. The results show that they can considerably lower energy requirement besides a further reduction in CI. © 2012 American Institute of Chemical Engineers AIChE J, 59: 2015–2032, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13993" xmlns="http://purl.org/rss/1.0/"><title>Delay-range-dependent guaranteed cost control for batch processes with state delay</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13993</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Delay-range-dependent guaranteed cost control for batch processes with state delay</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Limin Wang, Shengyong Mo, Donghua Zhou, Furong Gao, Xi Chen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-18T12:57:54.791723-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13993</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13993</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13993</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/">2033</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2045</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A guaranteed cost control scheme is proposed for batch processes described by a two-dimensional (2-D) system with uncertainties and interval time-varying delay. First, a 2-D controller, which includes a robust feedback control to ensure performances over time and an iterative learning control to improve the tracking performance from cycle to cycle, is formulated. The guaranteed cost law concept of the proposed 2-D controller is then introduced. Subsequently, by introducing the Lyapunov–Krasovskii function and adding a differential inequality to the Lyapunov function for the 2-D system, sufficient conditions for the existence of the robust guaranteed cost controller are derived in terms of matrix inequalities. A design procedure for the controller is also presented. Furthermore, a convex optimization problem with linear matrix inequality (LMI) constraints is formulated to design the optimal guaranteed cost controller that minimizes the upper bound of the closed-loop system cost. The proposed control law can stabilize the closed-loop system as well as guarantee <em>H<sub>∞</sub></em> performance level and a cost function with upper bounds for all admissible uncertainties. The results can be easily extended to the constant delay case. Finally, an illustrative example is given to demonstrate the effectiveness and advantages of the proposed 2-D design approach. © 2013 American Institute of Chemical Engineers AIChE J, 59: 2033–2045, 2013</p></div>
]]></content:encoded><description>
A guaranteed cost control scheme is proposed for batch processes described by a two-dimensional (2-D) system with uncertainties and interval time-varying delay. First, a 2-D controller, which includes a robust feedback control to ensure performances over time and an iterative learning control to improve the tracking performance from cycle to cycle, is formulated. The guaranteed cost law concept of the proposed 2-D controller is then introduced. Subsequently, by introducing the Lyapunov–Krasovskii function and adding a differential inequality to the Lyapunov function for the 2-D system, sufficient conditions for the existence of the robust guaranteed cost controller are derived in terms of matrix inequalities. A design procedure for the controller is also presented. Furthermore, a convex optimization problem with linear matrix inequality (LMI) constraints is formulated to design the optimal guaranteed cost controller that minimizes the upper bound of the closed-loop system cost. The proposed control law can stabilize the closed-loop system as well as guarantee H∞ performance level and a cost function with upper bounds for all admissible uncertainties. The results can be easily extended to the constant delay case. Finally, an illustrative example is given to demonstrate the effectiveness and advantages of the proposed 2-D design approach. © 2013 American Institute of Chemical Engineers AIChE J, 59: 2033–2045, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14010" xmlns="http://purl.org/rss/1.0/"><title>Applicability domain of soft sensor models based on one-class support vector machine</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14010</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Applicability domain of soft sensor models based on one-class support vector machine</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hiromasa Kaneko, Kimito Funatsu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-18T18:21:27.216676-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14010</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14010</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14010</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/">2046</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2050</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Soft sensors are widely used to estimate process variables that are difficult to measure online. By using soft sensors, analyzer faults can be detected by estimation errors. However, it is difficult to detect abnormal data and determine the reasons because estimation errors increase not only due to analyzer faults but also due to variations caused by changes in the state of chemical plants. To separate those factors, we previously proposed to construct the relationships between distances to soft sensor models (DMs) and the accuracy of prediction of the models quantitatively and estimate the prediction accuracy of new data online. In this article, we used a one-class support vector machine (OCSVM) to estimate data density and the output of an OCSVM as a DM. The proposed method was applied to real industrial data and the superiority of the proposed DM to the traditional ones was demonstrated by comparing their results. © 2013 American Institute of Chemical Engineers AIChE J, 59: 2046–2050, 2013</p></div>
]]></content:encoded><description>
Soft sensors are widely used to estimate process variables that are difficult to measure online. By using soft sensors, analyzer faults can be detected by estimation errors. However, it is difficult to detect abnormal data and determine the reasons because estimation errors increase not only due to analyzer faults but also due to variations caused by changes in the state of chemical plants. To separate those factors, we previously proposed to construct the relationships between distances to soft sensor models (DMs) and the accuracy of prediction of the models quantitatively and estimate the prediction accuracy of new data online. In this article, we used a one-class support vector machine (OCSVM) to estimate data density and the output of an OCSVM as a DM. The proposed method was applied to real industrial data and the superiority of the proposed DM to the traditional ones was demonstrated by comparing their results. © 2013 American Institute of Chemical Engineers AIChE J, 59: 2046–2050, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13991" xmlns="http://purl.org/rss/1.0/"><title>A thermal-flywheel approach to distributed temperature control in microchannel reactors</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13991</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A thermal-flywheel approach to distributed temperature control in microchannel reactors</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Richard C. Pattison, Michael Baldea</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-24T08:41:23.007463-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13991</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13991</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13991</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/">2051</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2061</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Microchannel reactors are a promising route for monetizing distributed natural gas resources. However, intensification and miniaturization represent a significant challenge for reactor control. Focusing on autothermal methane-steam reforming reactors, a novel microchannel reactor temperature control strategy based on confining a layer of phase-change material (PCM) between the reactor plates is introduced. Melting-solidification cycles, which occur with latent heat exchange at constant temperature, allow the PCM layer to act as an energy storage buffer—a “thermal flywheel”—constituting a distributed controller that mitigates temperature excursions caused by fluctuations in feedstock quality. A novel stochastic optimization algorithm for selecting the PCM layer thickness (i.e., distributed controller “tuning”) is introduced. Furthermore, a hierarchical control structure, whereby the PCM layer is complemented by a supervisory controller that addresses persistent disturbances, is proposed. The proposed concepts are illustrated in a comprehensive case study using a detailed two-dimensional reactor model. © 2013 American Institute of Chemical Engineers AIChE J, 59: 2051–2061, 2013</p></div>
]]></content:encoded><description>
Microchannel reactors are a promising route for monetizing distributed natural gas resources. However, intensification and miniaturization represent a significant challenge for reactor control. Focusing on autothermal methane-steam reforming reactors, a novel microchannel reactor temperature control strategy based on confining a layer of phase-change material (PCM) between the reactor plates is introduced. Melting-solidification cycles, which occur with latent heat exchange at constant temperature, allow the PCM layer to act as an energy storage buffer—a “thermal flywheel”—constituting a distributed controller that mitigates temperature excursions caused by fluctuations in feedstock quality. A novel stochastic optimization algorithm for selecting the PCM layer thickness (i.e., distributed controller “tuning”) is introduced. Furthermore, a hierarchical control structure, whereby the PCM layer is complemented by a supervisory controller that addresses persistent disturbances, is proposed. The proposed concepts are illustrated in a comprehensive case study using a detailed two-dimensional reactor model. © 2013 American Institute of Chemical Engineers AIChE J, 59: 2051–2061, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13989" xmlns="http://purl.org/rss/1.0/"><title>Liquid Fuels from Alternative Carbon Sources Minimizing Carbon Dioxide Emissions</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13989</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Liquid Fuels from Alternative Carbon Sources Minimizing Carbon Dioxide Emissions</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Matthew J. Metzger, Benjamin J. Glasser, Bilal Patel, James Fox, Baraka Celestin Sempuga, Diane Hildebrandt, David Glasser</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-19T17:00:12.595353-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13989</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13989</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13989</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/">2062</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2078</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The energy needs of the world continue to grow, as does the resulting environmental impact. Policy makers continue to call for alternative energies to replace today's petroleum-based liquid fuels. However, liquid fuels have significant advantages, and it is probably unwise to abandon the existing infrastructure without appropriately exploring alternatives to lessen the environmental burden of producing liquid fuels. Biomass and coal are often proposed as alternatives to petroleum-based carbon sources, but those processes lose a significant amount of their potential product to unwanted carbon dioxide emissions. However, combining biomass and coal with cleaner natural gas yields processes with less environmental impact to produce liquid fuels with small, zero, or even negative carbon dioxide emissions. Our process synthesis approach is applied to commonly encountered liquid fuel production methods to identify promising routes and to establish feasibility limits on those less promising alternatives. © 2013 American Institute of Chemical Engineers AIChE J, 59: 2062–2078, 2013</p></div>
]]></content:encoded><description>
The energy needs of the world continue to grow, as does the resulting environmental impact. Policy makers continue to call for alternative energies to replace today's petroleum-based liquid fuels. However, liquid fuels have significant advantages, and it is probably unwise to abandon the existing infrastructure without appropriately exploring alternatives to lessen the environmental burden of producing liquid fuels. Biomass and coal are often proposed as alternatives to petroleum-based carbon sources, but those processes lose a significant amount of their potential product to unwanted carbon dioxide emissions. However, combining biomass and coal with cleaner natural gas yields processes with less environmental impact to produce liquid fuels with small, zero, or even negative carbon dioxide emissions. Our process synthesis approach is applied to commonly encountered liquid fuel production methods to identify promising routes and to establish feasibility limits on those less promising alternatives. © 2013 American Institute of Chemical Engineers AIChE J, 59: 2062–2078, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13969" xmlns="http://purl.org/rss/1.0/"><title>Aromatics from Lignocellulosic Biomass: Economic Analysis of the Production of p-Xylene from 5-Hydroxymethylfurfural</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13969</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Aromatics from Lignocellulosic Biomass: Economic Analysis of the Production of p-Xylene from 5-Hydroxymethylfurfural</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Zhaojia Lin, Marianthi Ierapetritou, Vladimiros Nikolakis</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-20T13:42:49.859031-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13969</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13969</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13969</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/">2079</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2087</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A novel production of biobased p-xylene from hydroxymethylfurfual has been investigated and presented. This is an important part of a process for the production of aromatics from lignocellulosic biomass. The detailed flow sheets are designed based on laboratory experiments by Leshkov et al. and William et al. and economic analysis has been performed. The minimum biobased p-xylene cost is estimated as $3,962/metric ton, of which the main contribution comes from the HMF cost. Sensitivity analysis has been used to assess the impact of uncertainties of economic parameters and also to determine the most significant reaction factor in the technological development, i.e., selectivity and conversion. It has been shown that high selectivity is favored at the same yield. © 2013 American Institute of Chemical Engineers AIChE J, 59: 2079–2087, 2013</p></div>
]]></content:encoded><description>
A novel production of biobased p-xylene from hydroxymethylfurfual has been investigated and presented. This is an important part of a process for the production of aromatics from lignocellulosic biomass. The detailed flow sheets are designed based on laboratory experiments by Leshkov et al. and William et al. and economic analysis has been performed. The minimum biobased p-xylene cost is estimated as $3,962/metric ton, of which the main contribution comes from the HMF cost. Sensitivity analysis has been used to assess the impact of uncertainties of economic parameters and also to determine the most significant reaction factor in the technological development, i.e., selectivity and conversion. It has been shown that high selectivity is favored at the same yield. © 2013 American Institute of Chemical Engineers AIChE J, 59: 2079–2087, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13981" xmlns="http://purl.org/rss/1.0/"><title>Decanter Anomaly</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13981</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Decanter Anomaly</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">William L. Luyben</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-26T21:22:30.651428-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13981</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13981</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13981</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/">2088</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2095</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A counter-intuitive decanter level control structure was reported in an earlier article which the aqueous level controller had to use reverse action for stable control. The Aspen model used in this study was the simple Decanter model, which assumes that there are only two liquid phases and pressure remains constant. This article presents results when the alternative Flash3 model is used. The aqueous level controller with direct action works well. © 2012 American Institute of Chemical Engineers AIChE J, 59: 2088–2095, 2013</p></div>
]]></content:encoded><description>
A counter-intuitive decanter level control structure was reported in an earlier article which the aqueous level controller had to use reverse action for stable control. The Aspen model used in this study was the simple Decanter model, which assumes that there are only two liquid phases and pressure remains constant. This article presents results when the alternative Flash3 model is used. The aqueous level controller with direct action works well. © 2012 American Institute of Chemical Engineers AIChE J, 59: 2088–2095, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13960" xmlns="http://purl.org/rss/1.0/"><title>Selective conversion of glucose into lactic acid and acetic acid with copper oxide under hydrothermal conditions</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13960</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Selective conversion of glucose into lactic acid and acetic acid with copper oxide under hydrothermal conditions</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yuanqing Wang, Fangming Jin, Mitsuru Sasaki, Wahyudiono, Fengwen Wang, Zhenzi Jing, Motonobu Goto</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-07T10:49:01.4525-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13960</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13960</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13960</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, Kinetics, and Catalysis</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2096</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2104</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Biomass as a source for chemicals production attracts growing attention due to the decreasing storage of fossil fuels and global warming caused by emission of CO<sub>2</sub>. In this study, conversion of glucose with copper oxide (CuO) was studied under alkaline hydrothermal conditions using a batch reactor and continuous flow reactor. CuO, as an oxidant, greatly improves the yields of lactic acid (LA) and acetic acid from glucose and was reduced into Cu<sub>2</sub>O and Cu. Selective production of LA with the highest yield of 59% and acetic acid with the highest yield of 32% can be achieved by controlling reaction time, temperature, and addition of CuO. A possible mechanism of conversion of glucose with CuO was proposed. © 2012 American Institute of Chemical Engineers AIChE J, 59: 2096–2104, 2013</p></div>
]]></content:encoded><description>
Biomass as a source for chemicals production attracts growing attention due to the decreasing storage of fossil fuels and global warming caused by emission of CO2. In this study, conversion of glucose with copper oxide (CuO) was studied under alkaline hydrothermal conditions using a batch reactor and continuous flow reactor. CuO, as an oxidant, greatly improves the yields of lactic acid (LA) and acetic acid from glucose and was reduced into Cu2O and Cu. Selective production of LA with the highest yield of 59% and acetic acid with the highest yield of 32% can be achieved by controlling reaction time, temperature, and addition of CuO. A possible mechanism of conversion of glucose with CuO was proposed. © 2012 American Institute of Chemical Engineers AIChE J, 59: 2096–2104, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13979" xmlns="http://purl.org/rss/1.0/"><title>Hydrogen Production by Sorption-Enhanced Steam Glycerol Reforming: Sorption Kinetics and Reactor Simulation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13979</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Hydrogen Production by Sorption-Enhanced Steam Glycerol Reforming: Sorption Kinetics and Reactor Simulation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ion Iliuta, Hamid R. Radfarnia, Maria C. Iliuta</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-26T16:10:34.428046-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13979</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13979</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13979</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, Kinetics and Catalysis</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2105</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2118</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Sorption-enhanced glycerol reforming, an integrated process involving glycerol catalytic steam reforming and <em>in situ</em> CO<sub>2</sub> removal, offers a promising alternative for single-stage hydrogen production with high purity, reducing the abundant glycerol by-product streams. This work investigates this process in a fixed-bed reactor, via a two-scale, nonisothermal, unsteady-state model, highlighting the effect of key operating parameters on the process performance. CO<sub>2</sub> adsorption kinetics was investigated experimentally and described by a mathematical reaction-rate model. The integrated process presents an opportunity to improve the economics of green hydrogen production via an enhanced thermal efficiency process, the exothermic CO<sub>2</sub> adsorption providing the heat to endothermic steam glycerol reforming, while reducing the capital cost by removing the processing steps required for subsequently CO<sub>2</sub> separation. The operational time of producing high-purity hydrogen can be enhanced by increasing the adsorbent/catalyst volume ratio, by adding steam to the reaction system and by increasing the inlet reactor temperature. © 2012 American Institute of Chemical Engineers AIChE J, 59: 2105–2118, 2013</p></div>
]]></content:encoded><description>
Sorption-enhanced glycerol reforming, an integrated process involving glycerol catalytic steam reforming and in situ CO2 removal, offers a promising alternative for single-stage hydrogen production with high purity, reducing the abundant glycerol by-product streams. This work investigates this process in a fixed-bed reactor, via a two-scale, nonisothermal, unsteady-state model, highlighting the effect of key operating parameters on the process performance. CO2 adsorption kinetics was investigated experimentally and described by a mathematical reaction-rate model. The integrated process presents an opportunity to improve the economics of green hydrogen production via an enhanced thermal efficiency process, the exothermic CO2 adsorption providing the heat to endothermic steam glycerol reforming, while reducing the capital cost by removing the processing steps required for subsequently CO2 separation. The operational time of producing high-purity hydrogen can be enhanced by increasing the adsorbent/catalyst volume ratio, by adding steam to the reaction system and by increasing the inlet reactor temperature. © 2012 American Institute of Chemical Engineers AIChE J, 59: 2105–2118, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13984" xmlns="http://purl.org/rss/1.0/"><title>Cross-Scale Modeling and Simulation of Coal Pyrolysis to Acetylene in Hydrogen Plasma Reactors</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13984</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Cross-Scale Modeling and Simulation of Coal Pyrolysis to Acetylene in Hydrogen Plasma Reactors</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Binhang Yan, Yi Cheng, Yong Jin</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-07T07:30:17.801805-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13984</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13984</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13984</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, Kinetics and Catalysis</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2119</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2133</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Coal pyrolysis to acetylene in hydrogen plasma is carried out under ultrahigh temperature and milliseconds residence time. To better understand the complex gas-particle reaction behavior, a comprehensive computational fluid dynamics with discrete phase model has been established, with special consideration of the particle-scale physics such as the heat conduction inside particle. The improved chemical percolation devolatilization model that incorporates the tar cracking reactions is adopted. The model predictions are in good agreement with the performances of two pilot-plant reactors. The simulations reveal the detailed unmeasurable information of gas phase and particle-scale behaviors, then point out the facts that coal devolatilization almost finishes in the first 100 mm of the reaction chamber and the optimal particle diameter is suggested to be 20–50 μm. The different reactor performances during the scale-up from 2- to 5-MW unit are analyzed based on the detailed simulation results in combination with the operational experience. © 2012 American Institute of Chemical Engineers AIChE J, 59: 2119–2133, 2013</p></div>
]]></content:encoded><description>
Coal pyrolysis to acetylene in hydrogen plasma is carried out under ultrahigh temperature and milliseconds residence time. To better understand the complex gas-particle reaction behavior, a comprehensive computational fluid dynamics with discrete phase model has been established, with special consideration of the particle-scale physics such as the heat conduction inside particle. The improved chemical percolation devolatilization model that incorporates the tar cracking reactions is adopted. The model predictions are in good agreement with the performances of two pilot-plant reactors. The simulations reveal the detailed unmeasurable information of gas phase and particle-scale behaviors, then point out the facts that coal devolatilization almost finishes in the first 100 mm of the reaction chamber and the optimal particle diameter is suggested to be 20–50 μm. The different reactor performances during the scale-up from 2- to 5-MW unit are analyzed based on the detailed simulation results in combination with the operational experience. © 2012 American Institute of Chemical Engineers AIChE J, 59: 2119–2133, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13985" xmlns="http://purl.org/rss/1.0/"><title>A Novel Approach to Well-Aligned TiO2 Nanotube Arrays and Their Enhanced Photocatalytic Performances</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13985</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A Novel Approach to Well-Aligned TiO2 Nanotube Arrays and Their Enhanced Photocatalytic Performances</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Weixin Zhang, Gongde Chen, Zeheng Yang, Chunyan Zeng</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-08T12:34:50.016792-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13985</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13985</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13985</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, Kinetics and Catalysis</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2134</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2144</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A simple route has been developed to prepare well-aligned TiO<sub>2</sub> nanotube arrays, which is based on outward coating of TiO<sub>2</sub> and inward etching of Cu(OH)<sub>2</sub> nanorod templates. Effects of annealing temperature and time on the crystal size and crystallinity of TiO<sub>2</sub> nanotube arrays and photocatalytic activities of TiO<sub>2</sub> nanotube arrays for degradation of Rhodamine B in aqueous solution have been investigated. The results indicate that the TiO<sub>2</sub> nanotube arrays annealed at 500°C for 2 h possessed an enhanced photocatalytic activity in comparison with the TiO<sub>2</sub> nanotube arrays without post heating and commercial anatase TiO<sub>2</sub> nanoparticle film and presented a good life cycle performance. Scale-up of the process has also been demonstrated. Our work opens a new avenue to fabricate free-standing TiO<sub>2</sub> nanotube arrays and demonstrates an excellent photocatalytic performance of the anatase TiO<sub>2</sub> nanotube arrays for wastewater treatment. © 2012 American Institute of Chemical Engineers AIChE J, 59: 2134–2144, 2013</p></div>
]]></content:encoded><description>
A simple route has been developed to prepare well-aligned TiO2 nanotube arrays, which is based on outward coating of TiO2 and inward etching of Cu(OH)2 nanorod templates. Effects of annealing temperature and time on the crystal size and crystallinity of TiO2 nanotube arrays and photocatalytic activities of TiO2 nanotube arrays for degradation of Rhodamine B in aqueous solution have been investigated. The results indicate that the TiO2 nanotube arrays annealed at 500°C for 2 h possessed an enhanced photocatalytic activity in comparison with the TiO2 nanotube arrays without post heating and commercial anatase TiO2 nanoparticle film and presented a good life cycle performance. Scale-up of the process has also been demonstrated. Our work opens a new avenue to fabricate free-standing TiO2 nanotube arrays and demonstrates an excellent photocatalytic performance of the anatase TiO2 nanotube arrays for wastewater treatment. © 2012 American Institute of Chemical Engineers AIChE J, 59: 2134–2144, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13987" xmlns="http://purl.org/rss/1.0/"><title>Initial thickness measurements and insights into crystal growth of methane hydrate film</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13987</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Initial thickness measurements and insights into crystal growth of methane hydrate film</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sheng-Li Li, Chang-Yu Sun, Bei Liu, Xiu-Jun Feng, Feng-Guang Li, Li-Tao Chen, Guang-Jin Chen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-14T21:03:58.334195-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13987</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13987</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13987</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, Kinetics and Catalysis</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2145</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2154</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The initial thickness of methane hydrate film was directly measured by suspending a single methane bubble in water at 274.0, 276.0, and 278.0 K. The results show that the initial hydrate film thickness decreases from tens of micrometers to about 10 µm with the subcooling increased from 0.5 K to about 3 K. When subcooling is higher than 1.0 K, all initial film thickness data measured under different temperatures vary inversely with the subcooling. Notable three-dimensional growths of hydrate crystals of different sizes and shapes at film front and emergence of new crystal were clearly observed at lower subcooling that resulting in the rougher surface of hydrate film and uncertainty of initial thickness measurement under lower subcooling. The hydrate film growth was dominated by film growth in thickness, not by lateral growth at low subcooling. The growth in thickness of hydrate shell covering one whole bubble surface was also investigated. © 2013 American Institute of Chemical Engineers AIChE J, 59: 2145–2154, 2013</p></div>
]]></content:encoded><description>
The initial thickness of methane hydrate film was directly measured by suspending a single methane bubble in water at 274.0, 276.0, and 278.0 K. The results show that the initial hydrate film thickness decreases from tens of micrometers to about 10 µm with the subcooling increased from 0.5 K to about 3 K. When subcooling is higher than 1.0 K, all initial film thickness data measured under different temperatures vary inversely with the subcooling. Notable three-dimensional growths of hydrate crystals of different sizes and shapes at film front and emergence of new crystal were clearly observed at lower subcooling that resulting in the rougher surface of hydrate film and uncertainty of initial thickness measurement under lower subcooling. The hydrate film growth was dominated by film growth in thickness, not by lateral growth at low subcooling. The growth in thickness of hydrate shell covering one whole bubble surface was also investigated. © 2013 American Institute of Chemical Engineers AIChE J, 59: 2145–2154, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13994" xmlns="http://purl.org/rss/1.0/"><title>Quantitative analysis of gas hydrates using Raman spectroscopy</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13994</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Quantitative analysis of gas hydrates using Raman spectroscopy</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Junfeng Qin, Werner F. Kuhs</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-22T12:57:36.53609-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13994</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13994</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13994</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Reaction Engineering, Kinetics and Catalysis</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2155</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2167</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A calibration protocol to quantify the compositional information of gas hydrates using Raman spectroscopy is proposed. Structure I pure CH<sub>4</sub>-, CO<sub>2</sub>- and C<sub>2</sub>H<sub>6</sub>-hydrates in their deuterated and hydrogenated forms with known cage occupancies were investigated by Raman spectroscopy. Raman scattering cross sections of CH<sub>4</sub> in the large and small cages were found to be very similar, but not identical. Some C<sub>2</sub>H<sub>6</sub> bands of C<sub>2</sub>H<sub>6</sub>-hydrate were tentatively reassigned or newly reported and assigned. Our results show that the relative cross sections of guest vibrational modes in the deuterated hydrate are in agreement with those in the hydrogenated hydrate, whereas they are considerably different from those in fluid phase. Using our Raman quantification factors, the relative cage occupancies can now be determined more reliably in CH<sub>4</sub>-hydrates. Moreover, with additional assumptions, the absolute cage occupancies, the bulk guest composition and hydration number of pure or mixed gas hydrates become accessible by Raman spectroscopy. © 2013 American Institute of Chemical Engineers AIChE J, 59: 2155–2167, 2013</p></div>
]]></content:encoded><description>
A calibration protocol to quantify the compositional information of gas hydrates using Raman spectroscopy is proposed. Structure I pure CH4-, CO2- and C2H6-hydrates in their deuterated and hydrogenated forms with known cage occupancies were investigated by Raman spectroscopy. Raman scattering cross sections of CH4 in the large and small cages were found to be very similar, but not identical. Some C2H6 bands of C2H6-hydrate were tentatively reassigned or newly reported and assigned. Our results show that the relative cross sections of guest vibrational modes in the deuterated hydrate are in agreement with those in the hydrogenated hydrate, whereas they are considerably different from those in fluid phase. Using our Raman quantification factors, the relative cage occupancies can now be determined more reliably in CH4-hydrates. Moreover, with additional assumptions, the absolute cage occupancies, the bulk guest composition and hydration number of pure or mixed gas hydrates become accessible by Raman spectroscopy. © 2013 American Institute of Chemical Engineers AIChE J, 59: 2155–2167, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13967" xmlns="http://purl.org/rss/1.0/"><title>Theoretical and experimental investigation on the characteristics of fly-ash scrubbing in a fixed valve tray column</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13967</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Theoretical and experimental investigation on the characteristics of fly-ash scrubbing in a fixed valve tray column</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Qingli Wang, Xueli Chen, Xin Gong</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-07T11:14:25.978051-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13967</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13967</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13967</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separations: Materials, Devices and Processes</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2168</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2178</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The goal of this study is to evaluate the performance of a fixed valve tray column designed to remove fly-ash particles. A series of experiments were carried out at room temperature to demonstrate the collection efficiency of a fixed valve tray column at different gas and liquid superficial velocities. The fly-ash particles removal characteristics of the fixed valve tray column were evaluated by measuring variations of concentration and size distribution of particles in the outlet. The mechanism of particle removal in this turbulent dispersion system was theoretically analyzed on the basis of diffusion, interception, sedimentation and impaction, and a model was proposed to predict the collection efficiency. The results show that the simulation results agree well with the experimental data. In contrast to most of the conventional models, the present model is capable of evaluating the effects of bubble hydrodynamics, system property, and operation conditions on the collection efficiency. The model is expected to guide effectively the design and operation of valve tray washing columns, which is widely applied nowadays. © 2012 American Institute of Chemical Engineers AIChE J, 59: 2168–2178, 2013</p></div>
]]></content:encoded><description>
The goal of this study is to evaluate the performance of a fixed valve tray column designed to remove fly-ash particles. A series of experiments were carried out at room temperature to demonstrate the collection efficiency of a fixed valve tray column at different gas and liquid superficial velocities. The fly-ash particles removal characteristics of the fixed valve tray column were evaluated by measuring variations of concentration and size distribution of particles in the outlet. The mechanism of particle removal in this turbulent dispersion system was theoretically analyzed on the basis of diffusion, interception, sedimentation and impaction, and a model was proposed to predict the collection efficiency. The results show that the simulation results agree well with the experimental data. In contrast to most of the conventional models, the present model is capable of evaluating the effects of bubble hydrodynamics, system property, and operation conditions on the collection efficiency. The model is expected to guide effectively the design and operation of valve tray washing columns, which is widely applied nowadays. © 2012 American Institute of Chemical Engineers AIChE J, 59: 2168–2178, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13966" xmlns="http://purl.org/rss/1.0/"><title>Micropore size estimation on gas separation membranes: A study in experimental and molecular dynamics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13966</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Micropore size estimation on gas separation membranes: A study in experimental and molecular dynamics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Tomohisa Yoshioka, Masakoto Kanezashi, Toshinori Tsuru</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-27T02:10:31.016198-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13966</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13966</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13966</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separations: Materials, Devices, and Processes</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2179</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2194</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The effect of the gas molecular size and its affinity to the pore surface on gas permeation properties through the ceramic membranes was studied by both the gas permeation experiments and gas permeation simulations using a nonequilibrium molecular dynamics (MD) technique. A modified gas permeation model equation based on the gas translation (GT) mechanism was presented. MD simulation revealed that the effective diffusion length in a micropore depended on the gas molecular size, and the pre-exponential coefficient of a modified GT model equation showed good correlation with the kinetic diameter of the gas molecules. Also presented is a simple method to estimate the mean pore size of microporous membranes. The estimated pore sizes were consistent with observed kinetic diameter dependencies of gas permeance for real silica membranes. The pore size of a Deca-Dodecasil 3R (DDR) zeolite membrane was also reasonably estimated at ∼0.4 nm from the reported gas permeation data. © 2012 American Institute of Chemical Engineers AIChE J, 59: 2179–2194, 2013</p></div>
]]></content:encoded><description>
The effect of the gas molecular size and its affinity to the pore surface on gas permeation properties through the ceramic membranes was studied by both the gas permeation experiments and gas permeation simulations using a nonequilibrium molecular dynamics (MD) technique. A modified gas permeation model equation based on the gas translation (GT) mechanism was presented. MD simulation revealed that the effective diffusion length in a micropore depended on the gas molecular size, and the pre-exponential coefficient of a modified GT model equation showed good correlation with the kinetic diameter of the gas molecules. Also presented is a simple method to estimate the mean pore size of microporous membranes. The estimated pore sizes were consistent with observed kinetic diameter dependencies of gas permeance for real silica membranes. The pore size of a Deca-Dodecasil 3R (DDR) zeolite membrane was also reasonably estimated at ∼0.4 nm from the reported gas permeation data. © 2012 American Institute of Chemical Engineers AIChE J, 59: 2179–2194, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13970" xmlns="http://purl.org/rss/1.0/"><title>Enhancement of CO2 Adsorption and CO2/N2 Selectivity on ZIF-8 via Postsynthetic Modification</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13970</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Enhancement of CO2 Adsorption and CO2/N2 Selectivity on ZIF-8 via Postsynthetic Modification</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Zhijuan Zhang, Shikai Xian, Qibin Xia, Haihui Wang, Zhong Li, Jing Li</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-11T16:19:59.304844-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13970</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13970</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13970</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separations: Materials, Devices and Processes</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2195</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2206</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Imidazolate framework ZIF-8 is modified via postsynthetic method using etheylenediamine to improve its adsorption performance toward CO<sub>2</sub>. Results show that the BET surface area of the modified ZIF-8 (ED-ZIF-8) increases by 39%, and its adsorption capacity of CO<sub>2</sub> per surface area is almost two times of that on ZIF-8 at 298 K and 25 bar. H<sub>2</sub>O uptake on the ED-ZIF-8 become obviously lower compared to the ZIF-8. The ED-ZIF-8 selectivity for CO<sub>2</sub>/N<sub>2</sub> adsorption gets significantly improved, and is up to 23 and 13.9 separately at 0.1 and 0.5 bar, being almost twice of those of the ZIF-8. The isosteric heat of CO<sub>2</sub> adsorption (Q<sub>st</sub>) on the ED-ZIF-8 becomes higher, while Q<sub>st</sub> of N<sub>2</sub> gets slightly lower compared to those on the ZIF-8 Furthermore, it suggests that the postsynthetic modification of the ZIF-8 not only improves its adsorption capacity of CO<sub>2</sub> greatly, but also enhances its adsorption selectivity for CO<sub>2</sub>/N<sub>2</sub>/H<sub>2</sub>O significantly. ©2013 American Institute of Chemical Engineers AIChE J, 59: 2195–2206, 2013</p></div>
]]></content:encoded><description>
Imidazolate framework ZIF-8 is modified via postsynthetic method using etheylenediamine to improve its adsorption performance toward CO2. Results show that the BET surface area of the modified ZIF-8 (ED-ZIF-8) increases by 39%, and its adsorption capacity of CO2 per surface area is almost two times of that on ZIF-8 at 298 K and 25 bar. H2O uptake on the ED-ZIF-8 become obviously lower compared to the ZIF-8. The ED-ZIF-8 selectivity for CO2/N2 adsorption gets significantly improved, and is up to 23 and 13.9 separately at 0.1 and 0.5 bar, being almost twice of those of the ZIF-8. The isosteric heat of CO2 adsorption (Qst) on the ED-ZIF-8 becomes higher, while Qst of N2 gets slightly lower compared to those on the ZIF-8 Furthermore, it suggests that the postsynthetic modification of the ZIF-8 not only improves its adsorption capacity of CO2 greatly, but also enhances its adsorption selectivity for CO2/N2/H2O significantly. ©2013 American Institute of Chemical Engineers AIChE J, 59: 2195–2206, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14103" xmlns="http://purl.org/rss/1.0/"><title>Carbon dioxide separation and dry reforming of methane for synthesis of syngas by a dual-phase membrane reactor</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14103</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Carbon dioxide separation and dry reforming of methane for synthesis of syngas by a dual-phase membrane reactor</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Matthew Anderson, Y.S. Lin</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-08T09:41:35.949547-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14103</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14103</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14103</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separations: Materials, Devices and Processes</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2207</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2218</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>High-temperature CO<sub>2</sub> selective membranes offer potential for use to separate flue gas and produce a warm, pure CO<sub>2</sub> stream as a chemical feedstock. The coupling of separation of CO<sub>2</sub> by a ceramic–carbonate dual-phase membrane with dry reforming of CH<sub>4</sub> to produce syngas is reported. CO<sub>2</sub> permeation and the dry reforming reaction performance of the membrane reactor were experimentally studied with a CO<sub>2</sub>–N<sub>2</sub> mixture as the feed and CH<sub>4</sub> as the sweep gas passing through either an empty permeation chamber or one that was packed with a solid catalyst. CO<sub>2</sub> permeation flux through the membrane matches the rate of dry reforming of methane using a 10% Ni/γ-alumina catalyst at temperatures above 750°C. At 850°C under the reaction conditions, the membrane reactor gives a CO<sub>2</sub> permeation flux of 0.17 mL min<sup>−1</sup> cm<sup>−2</sup>, hydrogen production rate of 0.3 mL min<sup>−1</sup> cm<sup>−2</sup> with a H<sub>2</sub> to CO formation ratio of about 1, and conversion of CO<sub>2</sub> and CH<sub>4</sub>, respectively, of 88.5 and 8.1%. © 2013 American Institute of Chemical Engineers AIChE J, 59: 2207–2218, 2013</p></div>
]]></content:encoded><description>
High-temperature CO2 selective membranes offer potential for use to separate flue gas and produce a warm, pure CO2 stream as a chemical feedstock. The coupling of separation of CO2 by a ceramic–carbonate dual-phase membrane with dry reforming of CH4 to produce syngas is reported. CO2 permeation and the dry reforming reaction performance of the membrane reactor were experimentally studied with a CO2–N2 mixture as the feed and CH4 as the sweep gas passing through either an empty permeation chamber or one that was packed with a solid catalyst. CO2 permeation flux through the membrane matches the rate of dry reforming of methane using a 10% Ni/γ-alumina catalyst at temperatures above 750°C. At 850°C under the reaction conditions, the membrane reactor gives a CO2 permeation flux of 0.17 mL min−1 cm−2, hydrogen production rate of 0.3 mL min−1 cm−2 with a H2 to CO formation ratio of about 1, and conversion of CO2 and CH4, respectively, of 88.5 and 8.1%. © 2013 American Institute of Chemical Engineers AIChE J, 59: 2207–2218, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14109" xmlns="http://purl.org/rss/1.0/"><title>Drop-size distributions and spatial distributions in an annular centrifugal contactor</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14109</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Drop-size distributions and spatial distributions in an annular centrifugal contactor</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Nicholas B. Wyatt, Timothy J. O'Hern, Bion Shelden</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-16T09:11:03.926046-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.14109</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.14109</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.14109</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Separations: Materials, Devices and Processes</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2219</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2226</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Annular centrifugal contactors were developed as single, compact units utilized to transfer desired species between immiscible fluid phases. Critical to understanding the mass-transfer characteristics in the annular mixing region is a clear picture of the distribution of droplet sizes of the fluids involved. To date, very little experimental data appears in the literature. We fill that void by using laser fluorescence and optical methods to directly observe and measure drop-size distributions for a silicone oil/water system in a centrifugal contactor. The shape and characteristics of the log-normal distributions, including the Sauter mean diameter and distribution means, are elucidated in terms of rotor speed and organic phase fraction. The size distribution of entrained air bubbles is also examined. The results presented here will be invaluable in validating and expanding the predictive capacity of the many models that have been developed to describe the flow within these devices. Published 2013 American Institute of Chemical Engineers AIChE J, 59: 2219–2226, 2013</p></div>
]]></content:encoded><description>
Annular centrifugal contactors were developed as single, compact units utilized to transfer desired species between immiscible fluid phases. Critical to understanding the mass-transfer characteristics in the annular mixing region is a clear picture of the distribution of droplet sizes of the fluids involved. To date, very little experimental data appears in the literature. We fill that void by using laser fluorescence and optical methods to directly observe and measure drop-size distributions for a silicone oil/water system in a centrifugal contactor. The shape and characteristics of the log-normal distributions, including the Sauter mean diameter and distribution means, are elucidated in terms of rotor speed and organic phase fraction. The size distribution of entrained air bubbles is also examined. The results presented here will be invaluable in validating and expanding the predictive capacity of the many models that have been developed to describe the flow within these devices. Published 2013 American Institute of Chemical Engineers AIChE J, 59: 2219–2226, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13976" xmlns="http://purl.org/rss/1.0/"><title>Thermodynamic validation of 1-alkyl-3-methylimidazolium carboxylates as task-specific ionic liquids for H2S absorption</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13976</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Thermodynamic validation of 1-alkyl-3-methylimidazolium carboxylates as task-specific ionic liquids for H2S absorption</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Kuan Huang, Da-Niu Cai, Yong-Le Chen, You-Ting Wu, Xing-Bang Hu, Zhi-Bing Zhang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-18T09:58:41.181895-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13976</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13976</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13976</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Thermodynamics and Molecular-Scale Phenomena</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2227</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2235</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Solubilities of H<sub>2</sub>S in five 1-alkyl-3-methylimidazolium carboxylates ionic liquids (ILs) have been measured at temperatures from 293.15 to 333.15 K and pressures up to 350 kPa. It is shown that these ILs have significantly larger absorption capacities for H<sub>2</sub>S than those common ILs reported in the literature. The solubility is found to increase dramatically with the increasing alkalinity of the anions and slightly with the increasing length of the alkyl chains on the cations. It is further demonstrated that the absorption isotherms are typically nonideal. With the assumption of complex formation between H<sub>2</sub>S and ILs, a reaction equilibrium thermodynamic model is developed to correlate the experimental solubilities. The model favors a reaction mechanism of AB<sub>2</sub> type that two IL molecules interact with one H<sub>2</sub>S molecule. Thermodynamic parameters such as Henry's law constants, reaction equilibrium constants, and heat of complex formation are also calculated to evaluate the absorption process of H<sub>2</sub>S in these ILs. © 2012 American Institute of Chemical Engineers AIChE J, 59: 2227–2235, 2013</p></div>
]]></content:encoded><description>
Solubilities of H2S in five 1-alkyl-3-methylimidazolium carboxylates ionic liquids (ILs) have been measured at temperatures from 293.15 to 333.15 K and pressures up to 350 kPa. It is shown that these ILs have significantly larger absorption capacities for H2S than those common ILs reported in the literature. The solubility is found to increase dramatically with the increasing alkalinity of the anions and slightly with the increasing length of the alkyl chains on the cations. It is further demonstrated that the absorption isotherms are typically nonideal. With the assumption of complex formation between H2S and ILs, a reaction equilibrium thermodynamic model is developed to correlate the experimental solubilities. The model favors a reaction mechanism of AB2 type that two IL molecules interact with one H2S molecule. Thermodynamic parameters such as Henry's law constants, reaction equilibrium constants, and heat of complex formation are also calculated to evaluate the absorption process of H2S in these ILs. © 2012 American Institute of Chemical Engineers AIChE J, 59: 2227–2235, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13986" xmlns="http://purl.org/rss/1.0/"><title>Fluid-phase coexistence for the oxidation of CO2 expanded cyclohexane: Experiment, molecular simulation, and COSMO-SAC</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13986</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Fluid-phase coexistence for the oxidation of CO2 expanded cyclohexane: Experiment, molecular simulation, and COSMO-SAC</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">T. Merker, C.-M. Hsieh, S.-T. Lin, H. Hasse, J. Vrabec</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-25T09:57:09.77146-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13986</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13986</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13986</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Thermodynamics and Molecular-Scale Phenomena</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2236</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2250</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The gas solubility of pure oxygen and of pure carbon dioxide as well as of their gaseous mixture are measured in the ternary liquid mixture cyclohexane + cyclohexanone + cyclohexanol at 313.6 K with a high-pressure view-cell technique using the synthetic method. The new experimental data are used to assess the capability of molecular simulation and conductor-like screening model (COSMO)-SAC to predict multicomponent fluid-phase coexistence behavior. These methods are also compared systematically on the basis of experimental binary fluid-phase coexistence data. In that comparison also the Peng–Robinson (PR) equation of state is included as a reference. Molecular simulation and COSMO-SAC yield good results and are found to be far superior to the PR equation of state both in predictive and in adjusted mode. © 2013 American Institute of Chemical Engineers AIChE J, 59: 2236–2250, 2013</p></div>
]]></content:encoded><description>
The gas solubility of pure oxygen and of pure carbon dioxide as well as of their gaseous mixture are measured in the ternary liquid mixture cyclohexane + cyclohexanone + cyclohexanol at 313.6 K with a high-pressure view-cell technique using the synthetic method. The new experimental data are used to assess the capability of molecular simulation and conductor-like screening model (COSMO)-SAC to predict multicomponent fluid-phase coexistence behavior. These methods are also compared systematically on the basis of experimental binary fluid-phase coexistence data. In that comparison also the Peng–Robinson (PR) equation of state is included as a reference. Molecular simulation and COSMO-SAC yield good results and are found to be far superior to the PR equation of state both in predictive and in adjusted mode. © 2013 American Institute of Chemical Engineers AIChE J, 59: 2236–2250, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13973" xmlns="http://purl.org/rss/1.0/"><title>Experimental determination of the shear rate in a stirred tank with a non-newtonian fluid: Carbopol</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13973</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Experimental determination of the shear rate in a stirred tank with a non-newtonian fluid: Carbopol</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J.-C. Gabelle, J. Morchain, D. Anne-Archard, F. Augier, A. Liné</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-20T10:44:37.665892-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/aic.13973</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.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/aic.13973</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Faic.13973</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Transport Phenomena and Fluid Mechanics</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2251</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2266</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The local shear rate generated in a cylindrical tank equipped with a Rushton turbine was investigated using particle image velocimetry in a shear-thinning fluid (Carbopol). This non-Newtonian fluid was used in an attempt to mimic fermentation broths. Three Reynolds numbers corresponding to the transition regime were investigated. The hydrodynamics is analyzed, and the velocity field is decomposed by proper orthogonal decomposition into mean flow, organized motion, and turbulence. Then, the contributions of each flow structure to the total dissipation of kinetic energy are presented. The spatial heterogeneity of shear rate is discussed and a new expression is proposed for shear rate. This work shows that the local shear rate is highly heterogeneous in a tank. Future works will need to focus on other types of stirrer and investigate the effect of scaling up reactors on the shear rate heterogeneity. © 2012 American Institute of Chemical Engineers AIChE J, 59: 2251–2266, 2013</p></div>
]]></content:encoded><description>
The local shear rate generated in a cylindrical tank equipped with a Rushton turbine was investigated using particle image velocimetry in a shear-thinning fluid (Carbopol). This non-Newtonian fluid was used in an attempt to mimic fermentation broths. Three Reynolds numbers corresponding to the transition regime were investigated. The hydrodynamics is analyzed, and the velocity field is decomposed by proper orthogonal decomposition into mean flow, organized motion, and turbulence. Then, the contributions of each flow structure to the total dissipation of kinetic energy are presented. The spatial heterogeneity of shear rate is discussed and a new expression is proposed for shear rate. This work shows that the local shear rate is highly heterogeneous in a tank. Future works will need to focus on other types of stirrer and investigate the effect of scaling up reactors on the shear rate heterogeneity. © 2012 American Institute of Chemical Engineers AIChE J, 59: 2251–2266, 2013
</description></item></rdf:RDF>