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Please use this identifier to cite or link to this item: http://hdl.handle.net/2289/2270
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dc.contributor.authorGhosh, Sajal Kumar-
dc.contributor.authorGanapathy, R.-
dc.contributor.authorKrishnaswamy, Rema-
dc.contributor.authorBellare, J.-
dc.contributor.authorRaghunathan, V.A.-
dc.contributor.authorSood, A.K.-
dc.date.accessioned2007-04-23T09:30:13Z-
dc.date.available2007-04-23T09:30:13Z-
dc.date.issued2007-02-24-
dc.identifier.citationLangmuir, 2007, Vol. 23, p3606-3614en
dc.identifier.issn0743-7463-
dc.identifier.urihttp://hdl.handle.net/2289/2270-
dc.descriptionRestricted Access.en
dc.description.abstractWe report the observation of an intermediate mesh phase with rhombohedral symmetry, corresponding to the space group Rm, in a mixed surfactant system formed by the cationic surfactant cetyltrimethylammonium bromide (CTAB) and the organic salt 3-sodium-2-hydroxy naphthoate (SHN). It occurs between a random mesh phase () and a lamellar phase (L) at low temperatures; at higher temperatures, the phase transforms continuously into the L phase with an increasing surfactant concentration (s). To separate the effects of salt and s on the phase behavior, the ternary system consisting of cetyltrimethylammonium 3-hydroxy-naphthalene-2-carboxylate (CTAHN), sodium bromide (NaBr), and water was studied. The intermediate mesh phase is found in this system at high NaBr concentrations. The micellar aggregates, both in the intermediate and random mesh phases, are found to be made up of a two-dimensional network of rod-like segments, with three rods meeting at each node. The average mesh size increases with s, and the transition from the random mesh phase to the intermediate phase is found to occur when it is approximately 1.5 times the lamellar periodicity. The intermediate mesh phase is absent in the equimolar dodecyltrimethylammonium bromide (DTAB)-SHN system, indicating the role of the surfactant chain length in the formation of this phase. This system exhibits a random mesh phase over a very wide range of water content, with the average mesh size decreasing upon an increasing s, contrary to the trend seen in the CTAB-SHN system.en
dc.format.extent1033894 bytes-
dc.format.mimetypeapplication/pdf-
dc.language.isoenen
dc.publisherAmerican Chemical Societyen
dc.relation.urihttp://dx.doi.org/10.1021/la0631466en
dc.rights2007 American Chemical Societyen
dc.titleStructure of mesh phases in a cationic surfactant system with strongly bound counterionsen
dc.typeArticleen
Appears in Collections:Research Papers (SCM)

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