The Size of AOT Reverse Micelles
Reverse micelles (RMs) made from water and sodium bis(2-ethylhexyl) sulfosuccinate (AOT) are commonly studied experimentally as models of aqueous microenvironments. They are small enough for individual RMs to also be studied by molecular dynamics (MD) simulation, which yields detailed insight into...
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Veröffentlicht in: | The journal of physical chemistry. B 2016-11, Vol.120 (44), p.11337-11347 |
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description | Reverse micelles (RMs) made from water and sodium bis(2-ethylhexyl) sulfosuccinate (AOT) are commonly studied experimentally as models of aqueous microenvironments. They are small enough for individual RMs to also be studied by molecular dynamics (MD) simulation, which yields detailed insight into their structure and properties. Although RM size is determined by the water loading ratio (i.e., the molar ratio of water to AOT), experimental measurements of RM size are imprecise and inconsistent, which is problematic when seeking to understand the relationship between water loading ratio and RM size, and when designing models for study by MD simulation. Therefore, a systematic study of RM size was performed by MD simulation with the aims of determining the size of an RM for a given water loading ratio, and of reconciling the results with experimental measurements. Results for a water loading ratio of 7.5 indicate that the interaction energy between AOT anions and other system components is at a minimum when there are 62 AOT anions in each RM. The minimum is due to a combination of attractive and repulsive electrostatic interactions that vary with RM size and the dielectric effect of available water. Overall, the results agree with a detailed analysis of previously published experimental data over a wide range of water loading ratios, and help reconcile seemingly discrepant experimental results. In addition, water loss and gain from an RM is observed and the mechanism of water exchange is outlined. This kind of RM model, which faithfully reproduces experimental results, is essential for reliable insights into the properties of RM-encapsulated materials. |
doi_str_mv | 10.1021/acs.jpcb.6b06420 |
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They are small enough for individual RMs to also be studied by molecular dynamics (MD) simulation, which yields detailed insight into their structure and properties. Although RM size is determined by the water loading ratio (i.e., the molar ratio of water to AOT), experimental measurements of RM size are imprecise and inconsistent, which is problematic when seeking to understand the relationship between water loading ratio and RM size, and when designing models for study by MD simulation. Therefore, a systematic study of RM size was performed by MD simulation with the aims of determining the size of an RM for a given water loading ratio, and of reconciling the results with experimental measurements. Results for a water loading ratio of 7.5 indicate that the interaction energy between AOT anions and other system components is at a minimum when there are 62 AOT anions in each RM. The minimum is due to a combination of attractive and repulsive electrostatic interactions that vary with RM size and the dielectric effect of available water. Overall, the results agree with a detailed analysis of previously published experimental data over a wide range of water loading ratios, and help reconcile seemingly discrepant experimental results. In addition, water loss and gain from an RM is observed and the mechanism of water exchange is outlined. 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B</title><addtitle>J. Phys. Chem. B</addtitle><description>Reverse micelles (RMs) made from water and sodium bis(2-ethylhexyl) sulfosuccinate (AOT) are commonly studied experimentally as models of aqueous microenvironments. They are small enough for individual RMs to also be studied by molecular dynamics (MD) simulation, which yields detailed insight into their structure and properties. Although RM size is determined by the water loading ratio (i.e., the molar ratio of water to AOT), experimental measurements of RM size are imprecise and inconsistent, which is problematic when seeking to understand the relationship between water loading ratio and RM size, and when designing models for study by MD simulation. Therefore, a systematic study of RM size was performed by MD simulation with the aims of determining the size of an RM for a given water loading ratio, and of reconciling the results with experimental measurements. Results for a water loading ratio of 7.5 indicate that the interaction energy between AOT anions and other system components is at a minimum when there are 62 AOT anions in each RM. The minimum is due to a combination of attractive and repulsive electrostatic interactions that vary with RM size and the dielectric effect of available water. Overall, the results agree with a detailed analysis of previously published experimental data over a wide range of water loading ratios, and help reconcile seemingly discrepant experimental results. In addition, water loss and gain from an RM is observed and the mechanism of water exchange is outlined. This kind of RM model, which faithfully reproduces experimental results, is essential for reliable insights into the properties of RM-encapsulated materials.</description><subject>anions</subject><subject>Dioctyl Sulfosuccinic Acid - chemistry</subject><subject>electrostatic interactions</subject><subject>energy</subject><subject>Micelles</subject><subject>molecular dynamics</subject><subject>Molecular Dynamics Simulation</subject><subject>Particle Size</subject><subject>Water - chemistry</subject><issn>1520-6106</issn><issn>1520-5207</issn><issn>1520-5207</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><sourceid>EIF</sourceid><recordid>eNqFkc9LwzAUx4Mobk7vnqRHD3a-vKZpexHG8BcoA53n0KavrqNrZ7IO9K83c3XoQTyEBPL5fnnf92XslMOQA_LLVNvhfKmzocxACoQ91uchgu9OtN-9JQfZY0fWzgEwxFgesh5GUZBgkvSZN52R91x-kNcU3mgy9Z5oTcaS91hqqiqyx-ygSCtLJ909YC8319Pxnf8wub0fjx78VEi58jGhQMQyi6KQKIOIglyiToKoyCCLcx6khUaRB0hcJ7kQIeicolzGPM5CzDEYsKut77LNFpRrqlcmrdTSlIvUvKsmLdXvn7qcqddmrUIRJyi5MzjvDEzz1pJdqUVpNxnSmprWKgQAIYSL_S_K4yAUHAUHh8IW1aax1lCxm4iD2nSgXAdq04HqOnCSs59JdoLvpTvgYgt8SZvW1G6xf_t9Ai3fkPY</recordid><startdate>20161110</startdate><enddate>20161110</enddate><creator>Eskici, Gözde</creator><creator>Axelsen, Paul H</creator><general>American Chemical Society</general><scope>CGR</scope><scope>CUY</scope><scope>CVF</scope><scope>ECM</scope><scope>EIF</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><scope>7S9</scope><scope>L.6</scope><scope>5PM</scope></search><sort><creationdate>20161110</creationdate><title>The Size of AOT Reverse Micelles</title><author>Eskici, Gözde ; Axelsen, Paul H</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a466t-29e3486b775eeb07e3d62c937fb0b8d13afc24d32e1c9d4450cde7d6818b52d23</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>anions</topic><topic>Dioctyl Sulfosuccinic Acid - chemistry</topic><topic>electrostatic interactions</topic><topic>energy</topic><topic>Micelles</topic><topic>molecular dynamics</topic><topic>Molecular Dynamics Simulation</topic><topic>Particle Size</topic><topic>Water - chemistry</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Eskici, Gözde</creatorcontrib><creatorcontrib>Axelsen, Paul H</creatorcontrib><collection>Medline</collection><collection>MEDLINE</collection><collection>MEDLINE (Ovid)</collection><collection>MEDLINE</collection><collection>MEDLINE</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><collection>AGRICOLA</collection><collection>AGRICOLA - Academic</collection><collection>PubMed Central (Full Participant titles)</collection><jtitle>The journal of physical chemistry. B</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Eskici, Gözde</au><au>Axelsen, Paul H</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The Size of AOT Reverse Micelles</atitle><jtitle>The journal of physical chemistry. B</jtitle><addtitle>J. Phys. Chem. B</addtitle><date>2016-11-10</date><risdate>2016</risdate><volume>120</volume><issue>44</issue><spage>11337</spage><epage>11347</epage><pages>11337-11347</pages><issn>1520-6106</issn><issn>1520-5207</issn><eissn>1520-5207</eissn><abstract>Reverse micelles (RMs) made from water and sodium bis(2-ethylhexyl) sulfosuccinate (AOT) are commonly studied experimentally as models of aqueous microenvironments. They are small enough for individual RMs to also be studied by molecular dynamics (MD) simulation, which yields detailed insight into their structure and properties. Although RM size is determined by the water loading ratio (i.e., the molar ratio of water to AOT), experimental measurements of RM size are imprecise and inconsistent, which is problematic when seeking to understand the relationship between water loading ratio and RM size, and when designing models for study by MD simulation. Therefore, a systematic study of RM size was performed by MD simulation with the aims of determining the size of an RM for a given water loading ratio, and of reconciling the results with experimental measurements. Results for a water loading ratio of 7.5 indicate that the interaction energy between AOT anions and other system components is at a minimum when there are 62 AOT anions in each RM. The minimum is due to a combination of attractive and repulsive electrostatic interactions that vary with RM size and the dielectric effect of available water. Overall, the results agree with a detailed analysis of previously published experimental data over a wide range of water loading ratios, and help reconcile seemingly discrepant experimental results. In addition, water loss and gain from an RM is observed and the mechanism of water exchange is outlined. This kind of RM model, which faithfully reproduces experimental results, is essential for reliable insights into the properties of RM-encapsulated materials.</abstract><cop>United States</cop><pub>American Chemical Society</pub><pmid>27739299</pmid><doi>10.1021/acs.jpcb.6b06420</doi><tpages>11</tpages><oa>free_for_read</oa></addata></record> |
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subjects | anions Dioctyl Sulfosuccinic Acid - chemistry electrostatic interactions energy Micelles molecular dynamics Molecular Dynamics Simulation Particle Size Water - chemistry |
title | The Size of AOT Reverse Micelles |
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