Surface-Aggregate Shape Transformation
The structure of surfactant surface-aggregates can be controlled by mixing two surfactants which, individually, form different surface-aggregate structures. Using atomic force microscopy (AFM), we have found that mixtures of (dodecyldimethylammonio)propanesulfonate (DDAPS) and dodecyltrimethylammoni...
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Veröffentlicht in: | Langmuir 1996-11, Vol.12 (24), p.5915-5920 |
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creator | Ducker, William A Wanless, Erica J |
description | The structure of surfactant surface-aggregates can be controlled by mixing two surfactants which, individually, form different surface-aggregate structures. Using atomic force microscopy (AFM), we have found that mixtures of (dodecyldimethylammonio)propanesulfonate (DDAPS) and dodecyltrimethylammonium bromide (DTAB) at the interface between mica and aqueous solution form aggregates (“hemimicelles”) which have a length dictated by the proportion of each surfactant in the mixture. In pure DDAPS, the two axes of the aggregate parallel to the mica−solution interface are similar in length and similar to the diameter of a bulk micelle. As the mole fraction of DTAB in solution is increased, one axis of the surface aggregates increases while the other remains almost constant. In the limit of pure DTAB solutions, the aspect ratio is large (>10). The length of the mixed aggregates is not a linear function of the mole fraction of DTAB in bulk, but this can be partially rationalized on the basis of electrostatic interactions which concentrate DTA+ at the mica−solution interface at low bulk concentration. Both DTAB and DDAPS form approximately spherical aggregates in bulk solution, so the surface shape transformation cannot be accompanied by an analogous bulk transformation. |
doi_str_mv | 10.1021/la9605448 |
format | Article |
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Using atomic force microscopy (AFM), we have found that mixtures of (dodecyldimethylammonio)propanesulfonate (DDAPS) and dodecyltrimethylammonium bromide (DTAB) at the interface between mica and aqueous solution form aggregates (“hemimicelles”) which have a length dictated by the proportion of each surfactant in the mixture. In pure DDAPS, the two axes of the aggregate parallel to the mica−solution interface are similar in length and similar to the diameter of a bulk micelle. As the mole fraction of DTAB in solution is increased, one axis of the surface aggregates increases while the other remains almost constant. In the limit of pure DTAB solutions, the aspect ratio is large (>10). The length of the mixed aggregates is not a linear function of the mole fraction of DTAB in bulk, but this can be partially rationalized on the basis of electrostatic interactions which concentrate DTA+ at the mica−solution interface at low bulk concentration. 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Using atomic force microscopy (AFM), we have found that mixtures of (dodecyldimethylammonio)propanesulfonate (DDAPS) and dodecyltrimethylammonium bromide (DTAB) at the interface between mica and aqueous solution form aggregates (“hemimicelles”) which have a length dictated by the proportion of each surfactant in the mixture. In pure DDAPS, the two axes of the aggregate parallel to the mica−solution interface are similar in length and similar to the diameter of a bulk micelle. As the mole fraction of DTAB in solution is increased, one axis of the surface aggregates increases while the other remains almost constant. In the limit of pure DTAB solutions, the aspect ratio is large (>10). The length of the mixed aggregates is not a linear function of the mole fraction of DTAB in bulk, but this can be partially rationalized on the basis of electrostatic interactions which concentrate DTA+ at the mica−solution interface at low bulk concentration. Both DTAB and DDAPS form approximately spherical aggregates in bulk solution, so the surface shape transformation cannot be accompanied by an analogous bulk transformation.</description><subject>Chemistry</subject><subject>Exact sciences and technology</subject><subject>General and physical chemistry</subject><subject>Solid-liquid interface</subject><subject>Surface physical chemistry</subject><issn>0743-7463</issn><issn>1520-5827</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1996</creationdate><recordtype>article</recordtype><recordid>eNptj01LAzEQhoMoWKsH_0EPKnhYnc1nc5Rq_aCg2HoOYzKpW9tuSbag_96VlZ48zeF9Zt55GDst4aoEXl4v0WpQUg73WK9UHAo15Gaf9cBIURipxSE7ynkBAFZI22MX022K6Km4mc8TzbGhwfQDNzSYJVznWKcVNlW9PmYHEZeZTv5mn72N72ajh2LyfP84upkUKLhsioiEZQkQLA_GWyODD8Ia0CHIoN41Cc3B6MBVDBYkKSRPERVFIYAEiT677O76VOecKLpNqlaYvl0J7lfQ7QRb9qxjN5g9LmP7sK_yboG39sBNixUdVuWGvnYxpk-njTDKzV6mTo_g6fZ1PHSTlj_vePTZLeptWrfC_9T_AEbUaeI</recordid><startdate>19961127</startdate><enddate>19961127</enddate><creator>Ducker, William A</creator><creator>Wanless, Erica J</creator><general>American Chemical Society</general><scope>BSCLL</scope><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>19961127</creationdate><title>Surface-Aggregate Shape Transformation</title><author>Ducker, William A ; Wanless, Erica J</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a324t-faea1100d92d7c974dcd39706dd4d5b6e362076d25fd904e5aecefa5ef330e3e3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1996</creationdate><topic>Chemistry</topic><topic>Exact sciences and technology</topic><topic>General and physical chemistry</topic><topic>Solid-liquid interface</topic><topic>Surface physical chemistry</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ducker, William A</creatorcontrib><creatorcontrib>Wanless, Erica J</creatorcontrib><collection>Istex</collection><collection>Pascal-Francis</collection><collection>CrossRef</collection><jtitle>Langmuir</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ducker, William A</au><au>Wanless, Erica J</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Surface-Aggregate Shape Transformation</atitle><jtitle>Langmuir</jtitle><addtitle>Langmuir</addtitle><date>1996-11-27</date><risdate>1996</risdate><volume>12</volume><issue>24</issue><spage>5915</spage><epage>5920</epage><pages>5915-5920</pages><issn>0743-7463</issn><eissn>1520-5827</eissn><coden>LANGD5</coden><abstract>The structure of surfactant surface-aggregates can be controlled by mixing two surfactants which, individually, form different surface-aggregate structures. Using atomic force microscopy (AFM), we have found that mixtures of (dodecyldimethylammonio)propanesulfonate (DDAPS) and dodecyltrimethylammonium bromide (DTAB) at the interface between mica and aqueous solution form aggregates (“hemimicelles”) which have a length dictated by the proportion of each surfactant in the mixture. In pure DDAPS, the two axes of the aggregate parallel to the mica−solution interface are similar in length and similar to the diameter of a bulk micelle. As the mole fraction of DTAB in solution is increased, one axis of the surface aggregates increases while the other remains almost constant. In the limit of pure DTAB solutions, the aspect ratio is large (>10). The length of the mixed aggregates is not a linear function of the mole fraction of DTAB in bulk, but this can be partially rationalized on the basis of electrostatic interactions which concentrate DTA+ at the mica−solution interface at low bulk concentration. Both DTAB and DDAPS form approximately spherical aggregates in bulk solution, so the surface shape transformation cannot be accompanied by an analogous bulk transformation.</abstract><cop>Washington, DC</cop><pub>American Chemical Society</pub><doi>10.1021/la9605448</doi><tpages>6</tpages></addata></record> |
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subjects | Chemistry Exact sciences and technology General and physical chemistry Solid-liquid interface Surface physical chemistry |
title | Surface-Aggregate Shape Transformation |
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