Adsorption energies for a nanoporous carbon from gas–solid chromatography and molecular mechanics
Gas–solid chromatography was used to obtain second gas–solid virial coefficients, B 2 s , in the temperature range 342–613 K for methane, ethane, propane, butane, 2-methylpropane, chloromethane, chlorodifluoromethane, dichloromethane, and dichlorodifluoromethane. The adsorbent used was Carbosieve S-...
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creator | Rybolt, Thomas R. Ziegler, Katherine A. Thomas, Howard E. Boyd, Jennifer L. Ridgeway, Mark E. |
description | Gas–solid chromatography was used to obtain second gas–solid virial coefficients,
B
2
s
, in the temperature range 342–613 K for methane, ethane, propane, butane, 2-methylpropane, chloromethane, chlorodifluoromethane, dichloromethane, and dichlorodifluoromethane. The adsorbent used was Carbosieve S-III (Supelco), a carbon powder with fairly uniform, predominately 0.55 nm slit width pores and a N
2 BET surface area of 995 m
2/g. The temperature dependence of
B
2
s
was used to determine experimental values of the gas–solid interaction energy,
E
∗
, for each of these molecular adsorbates. MM2 and MM3 molecular mechanics calculations were used to determine the gas–solid interaction energy,
E
cal
∗
, for each of the molecules on various flat and nanoporous model surfaces. The flat model consisted of three parallel graphene layers with each graphene layer containing 127 interconnected benzene rings. The nanoporous model consisted of two sets of three parallel graphene layers adjacent to one another but separated to represent the pore diameter. A variety of calculated adsorption energies,
E
cal
∗
, were compared and correlated to the experimental
E
∗
values. It was determined that simple molecular mechanics could be used to calculate an attraction energy parameter between an adsorbed molecule and the carbon surface. The best correlation between the
E
cal
∗
and
E
∗
values was provided by a 0.50 nm nanoporous model using MM2 parameters. |
doi_str_mv | 10.1016/j.jcis.2005.08.057 |
format | Article |
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B
2
s
, in the temperature range 342–613 K for methane, ethane, propane, butane, 2-methylpropane, chloromethane, chlorodifluoromethane, dichloromethane, and dichlorodifluoromethane. The adsorbent used was Carbosieve S-III (Supelco), a carbon powder with fairly uniform, predominately 0.55 nm slit width pores and a N
2 BET surface area of 995 m
2/g. The temperature dependence of
B
2
s
was used to determine experimental values of the gas–solid interaction energy,
E
∗
, for each of these molecular adsorbates. MM2 and MM3 molecular mechanics calculations were used to determine the gas–solid interaction energy,
E
cal
∗
, for each of the molecules on various flat and nanoporous model surfaces. The flat model consisted of three parallel graphene layers with each graphene layer containing 127 interconnected benzene rings. The nanoporous model consisted of two sets of three parallel graphene layers adjacent to one another but separated to represent the pore diameter. A variety of calculated adsorption energies,
E
cal
∗
, were compared and correlated to the experimental
E
∗
values. It was determined that simple molecular mechanics could be used to calculate an attraction energy parameter between an adsorbed molecule and the carbon surface. The best correlation between the
E
cal
∗
and
E
∗
values was provided by a 0.50 nm nanoporous model using MM2 parameters.</description><identifier>ISSN: 0021-9797</identifier><identifier>EISSN: 1095-7103</identifier><identifier>DOI: 10.1016/j.jcis.2005.08.057</identifier><identifier>PMID: 16168430</identifier><identifier>CODEN: JCISA5</identifier><language>eng</language><publisher>San Diego, CA: Elsevier Inc</publisher><subject>Adsorption ; Adsorption energy ; carbon ; Chemistry ; Colloidal state and disperse state ; correlations of ; Exact sciences and technology ; formula omitted ; gas–solid ; gas–solid chromatography ; General and physical chemistry ; Henry's law ; Molecular mechanics surface energy ; Porous materials ; Surface physical chemistry ; Virial coefficients</subject><ispartof>Journal of colloid and interface science, 2006-04, Vol.296 (1), p.41-50</ispartof><rights>2005 Elsevier Inc.</rights><rights>2006 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c450t-fc68bbfd280a38a3a82900f33660a93a29a8c1c7140078e481b23d9bebc43acd3</citedby><cites>FETCH-LOGICAL-c450t-fc68bbfd280a38a3a82900f33660a93a29a8c1c7140078e481b23d9bebc43acd3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.sciencedirect.com/science/article/pii/S0021979705009082$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,776,780,3537,27901,27902,65306</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=17671108$$DView record in Pascal Francis$$Hfree_for_read</backlink><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/16168430$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Rybolt, Thomas R.</creatorcontrib><creatorcontrib>Ziegler, Katherine A.</creatorcontrib><creatorcontrib>Thomas, Howard E.</creatorcontrib><creatorcontrib>Boyd, Jennifer L.</creatorcontrib><creatorcontrib>Ridgeway, Mark E.</creatorcontrib><title>Adsorption energies for a nanoporous carbon from gas–solid chromatography and molecular mechanics</title><title>Journal of colloid and interface science</title><addtitle>J Colloid Interface Sci</addtitle><description>Gas–solid chromatography was used to obtain second gas–solid virial coefficients,
B
2
s
, in the temperature range 342–613 K for methane, ethane, propane, butane, 2-methylpropane, chloromethane, chlorodifluoromethane, dichloromethane, and dichlorodifluoromethane. The adsorbent used was Carbosieve S-III (Supelco), a carbon powder with fairly uniform, predominately 0.55 nm slit width pores and a N
2 BET surface area of 995 m
2/g. The temperature dependence of
B
2
s
was used to determine experimental values of the gas–solid interaction energy,
E
∗
, for each of these molecular adsorbates. MM2 and MM3 molecular mechanics calculations were used to determine the gas–solid interaction energy,
E
cal
∗
, for each of the molecules on various flat and nanoporous model surfaces. The flat model consisted of three parallel graphene layers with each graphene layer containing 127 interconnected benzene rings. The nanoporous model consisted of two sets of three parallel graphene layers adjacent to one another but separated to represent the pore diameter. A variety of calculated adsorption energies,
E
cal
∗
, were compared and correlated to the experimental
E
∗
values. It was determined that simple molecular mechanics could be used to calculate an attraction energy parameter between an adsorbed molecule and the carbon surface. The best correlation between the
E
cal
∗
and
E
∗
values was provided by a 0.50 nm nanoporous model using MM2 parameters.</description><subject>Adsorption</subject><subject>Adsorption energy</subject><subject>carbon</subject><subject>Chemistry</subject><subject>Colloidal state and disperse state</subject><subject>correlations of</subject><subject>Exact sciences and technology</subject><subject>formula omitted</subject><subject>gas–solid</subject><subject>gas–solid chromatography</subject><subject>General and physical chemistry</subject><subject>Henry's law</subject><subject>Molecular mechanics surface energy</subject><subject>Porous materials</subject><subject>Surface physical chemistry</subject><subject>Virial coefficients</subject><issn>0021-9797</issn><issn>1095-7103</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2006</creationdate><recordtype>article</recordtype><recordid>eNp9kMFu1DAQhi0EokvhBTggX-gt6ThOYkfiUlWUIlXiAmdrMnF2vUrsYGeReuMd-oY8CV7tCm49jTT6_l8zH2PvBZQCRHu9L_fkUlkBNCXoEhr1gm0EdE2hBMiXbANQiaJTnbpgb1LaAwjRNN1rdiFa0epawobRzZBCXFYXPLfexq2ziY8hcuQefVhCDIfECWOfgTGGmW8x_fn9lMLkBk67vME1bCMuu0eOfuBzmCwdJox8trRD7yi9Za9GnJJ9d56X7Mfd5--398XDty9fb28eCqobWIuRWt3341BpQKlRoq46gFHKtgXsJFYdahKkRA2gtK216Cs5dL3tqZZIg7xkV6feJYafB5tWM7tEdprQ2_yFaZUSldYqg9UJpBhSinY0S3QzxkcjwBzVmr05qjVHtQa0yWpz6MO5_dDPdvgfObvMwMczgIlwGiP6Y8c_TrVKCNCZ-3TibHbxy9loEjnryQ4uWlrNENxzd_wF6oKaDg</recordid><startdate>20060401</startdate><enddate>20060401</enddate><creator>Rybolt, Thomas R.</creator><creator>Ziegler, Katherine A.</creator><creator>Thomas, Howard E.</creator><creator>Boyd, Jennifer L.</creator><creator>Ridgeway, Mark E.</creator><general>Elsevier Inc</general><general>Elsevier</general><scope>IQODW</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope></search><sort><creationdate>20060401</creationdate><title>Adsorption energies for a nanoporous carbon from gas–solid chromatography and molecular mechanics</title><author>Rybolt, Thomas R. ; Ziegler, Katherine A. ; Thomas, Howard E. ; Boyd, Jennifer L. ; Ridgeway, Mark E.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c450t-fc68bbfd280a38a3a82900f33660a93a29a8c1c7140078e481b23d9bebc43acd3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2006</creationdate><topic>Adsorption</topic><topic>Adsorption energy</topic><topic>carbon</topic><topic>Chemistry</topic><topic>Colloidal state and disperse state</topic><topic>correlations of</topic><topic>Exact sciences and technology</topic><topic>formula omitted</topic><topic>gas–solid</topic><topic>gas–solid chromatography</topic><topic>General and physical chemistry</topic><topic>Henry's law</topic><topic>Molecular mechanics surface energy</topic><topic>Porous materials</topic><topic>Surface physical chemistry</topic><topic>Virial coefficients</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Rybolt, Thomas R.</creatorcontrib><creatorcontrib>Ziegler, Katherine A.</creatorcontrib><creatorcontrib>Thomas, Howard E.</creatorcontrib><creatorcontrib>Boyd, Jennifer L.</creatorcontrib><creatorcontrib>Ridgeway, Mark E.</creatorcontrib><collection>Pascal-Francis</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><jtitle>Journal of colloid and interface science</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Rybolt, Thomas R.</au><au>Ziegler, Katherine A.</au><au>Thomas, Howard E.</au><au>Boyd, Jennifer L.</au><au>Ridgeway, Mark E.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Adsorption energies for a nanoporous carbon from gas–solid chromatography and molecular mechanics</atitle><jtitle>Journal of colloid and interface science</jtitle><addtitle>J Colloid Interface Sci</addtitle><date>2006-04-01</date><risdate>2006</risdate><volume>296</volume><issue>1</issue><spage>41</spage><epage>50</epage><pages>41-50</pages><issn>0021-9797</issn><eissn>1095-7103</eissn><coden>JCISA5</coden><abstract>Gas–solid chromatography was used to obtain second gas–solid virial coefficients,
B
2
s
, in the temperature range 342–613 K for methane, ethane, propane, butane, 2-methylpropane, chloromethane, chlorodifluoromethane, dichloromethane, and dichlorodifluoromethane. The adsorbent used was Carbosieve S-III (Supelco), a carbon powder with fairly uniform, predominately 0.55 nm slit width pores and a N
2 BET surface area of 995 m
2/g. The temperature dependence of
B
2
s
was used to determine experimental values of the gas–solid interaction energy,
E
∗
, for each of these molecular adsorbates. MM2 and MM3 molecular mechanics calculations were used to determine the gas–solid interaction energy,
E
cal
∗
, for each of the molecules on various flat and nanoporous model surfaces. The flat model consisted of three parallel graphene layers with each graphene layer containing 127 interconnected benzene rings. The nanoporous model consisted of two sets of three parallel graphene layers adjacent to one another but separated to represent the pore diameter. A variety of calculated adsorption energies,
E
cal
∗
, were compared and correlated to the experimental
E
∗
values. It was determined that simple molecular mechanics could be used to calculate an attraction energy parameter between an adsorbed molecule and the carbon surface. The best correlation between the
E
cal
∗
and
E
∗
values was provided by a 0.50 nm nanoporous model using MM2 parameters.</abstract><cop>San Diego, CA</cop><pub>Elsevier Inc</pub><pmid>16168430</pmid><doi>10.1016/j.jcis.2005.08.057</doi><tpages>10</tpages></addata></record> |
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source | Elsevier ScienceDirect Journals Collection |
subjects | Adsorption Adsorption energy carbon Chemistry Colloidal state and disperse state correlations of Exact sciences and technology formula omitted gas–solid gas–solid chromatography General and physical chemistry Henry's law Molecular mechanics surface energy Porous materials Surface physical chemistry Virial coefficients |
title | Adsorption energies for a nanoporous carbon from gas–solid chromatography and molecular mechanics |
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