Surface and bulk properties of aqueous decyltrimethylammonium bromide–hexadecyltrimethylammonium bromide mixed system

The aqueous mixed system decyltrimethylammonium bromide (C 10TAB)–hexadecyltrimethylammonium bromide (C 16TAB) was studied by conductivity, ion-selective electrodes, surface tension, and fluorescence spectroscopy techniques. The mixture critical micelle concentration, cmc*, aggregation number, N ∗ ,...

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Veröffentlicht in:Journal of colloid and interface science 2007-10, Vol.314 (2), p.699-706
Hauptverfasser: Rodríguez, J.L., Sierra, M.B., Messina, P.V., Morini, M.A., Schulz, P.C., del Burgo, P., Junquera, E., Rodríguez, A., Aicart, E.
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container_issue 2
container_start_page 699
container_title Journal of colloid and interface science
container_volume 314
creator Rodríguez, J.L.
Sierra, M.B.
Messina, P.V.
Morini, M.A.
Schulz, P.C.
del Burgo, P.
Junquera, E.
Rodríguez, A.
Aicart, E.
description The aqueous mixed system decyltrimethylammonium bromide (C 10TAB)–hexadecyltrimethylammonium bromide (C 16TAB) was studied by conductivity, ion-selective electrodes, surface tension, and fluorescence spectroscopy techniques. The mixture critical micelle concentration, cmc*, aggregation number, N ∗ , and micelle molar conductivity, Λ M cmc , showed that the system aggregation is strongly nonideal. Both cmc* and N ∗ results were analyzed with two different procedures: (i) the regular solution theory on mixed micelles or Rubingh's theory, and (ii) by the determination of the partial critical micelle concentration of the amphiphile component i in the presence of a constant concentration of the other amphiphile component, cmc i ∗ . The Rubingh procedure gives micelles richer in C 16TAB than the overall mixtures, while procedure (ii) gives micelles having the same composition as in the complete surfactant mixture ( α C 10 TAB ). Mixed micelles are larger than pure surfactant ones, with nonspherical shape. Using a literature model, the cause of the synergistic effect seems to be a reduction of the hydrocarbon/water contact at the micelle surface when mixed micelles form. Conductivity and ion-selective electrodes indicate that highly ionized premicelles form immediately before the cmc*. The air/solution interface is strongly nonideal and much richer in C 16 TAB than the composition in the bulk. When micelles form there is a strong desorption from the air/solution interface because micelles are energetically favored when compared with the monolayer. The aqueous mixed system C 10TAB–C 16TAB was studied by conductivity, ion-selective electrodes, surface tension, and fluorescence spectroscopy. Results were analyzed by the regular solution theory, and by the partial critical micelle concentration of one component in the presence of a constant concentration of the other one.
doi_str_mv 10.1016/j.jcis.2007.06.010
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The mixture critical micelle concentration, cmc*, aggregation number, N ∗ , and micelle molar conductivity, Λ M cmc , showed that the system aggregation is strongly nonideal. Both cmc* and N ∗ results were analyzed with two different procedures: (i) the regular solution theory on mixed micelles or Rubingh's theory, and (ii) by the determination of the partial critical micelle concentration of the amphiphile component i in the presence of a constant concentration of the other amphiphile component, cmc i ∗ . The Rubingh procedure gives micelles richer in C 16TAB than the overall mixtures, while procedure (ii) gives micelles having the same composition as in the complete surfactant mixture ( α C 10 TAB ). Mixed micelles are larger than pure surfactant ones, with nonspherical shape. Using a literature model, the cause of the synergistic effect seems to be a reduction of the hydrocarbon/water contact at the micelle surface when mixed micelles form. Conductivity and ion-selective electrodes indicate that highly ionized premicelles form immediately before the cmc*. The air/solution interface is strongly nonideal and much richer in C 16 TAB than the composition in the bulk. When micelles form there is a strong desorption from the air/solution interface because micelles are energetically favored when compared with the monolayer. The aqueous mixed system C 10TAB–C 16TAB was studied by conductivity, ion-selective electrodes, surface tension, and fluorescence spectroscopy. 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The mixture critical micelle concentration, cmc*, aggregation number, N ∗ , and micelle molar conductivity, Λ M cmc , showed that the system aggregation is strongly nonideal. Both cmc* and N ∗ results were analyzed with two different procedures: (i) the regular solution theory on mixed micelles or Rubingh's theory, and (ii) by the determination of the partial critical micelle concentration of the amphiphile component i in the presence of a constant concentration of the other amphiphile component, cmc i ∗ . The Rubingh procedure gives micelles richer in C 16TAB than the overall mixtures, while procedure (ii) gives micelles having the same composition as in the complete surfactant mixture ( α C 10 TAB ). Mixed micelles are larger than pure surfactant ones, with nonspherical shape. Using a literature model, the cause of the synergistic effect seems to be a reduction of the hydrocarbon/water contact at the micelle surface when mixed micelles form. Conductivity and ion-selective electrodes indicate that highly ionized premicelles form immediately before the cmc*. The air/solution interface is strongly nonideal and much richer in C 16 TAB than the composition in the bulk. When micelles form there is a strong desorption from the air/solution interface because micelles are energetically favored when compared with the monolayer. The aqueous mixed system C 10TAB–C 16TAB was studied by conductivity, ion-selective electrodes, surface tension, and fluorescence spectroscopy. Results were analyzed by the regular solution theory, and by the partial critical micelle concentration of one component in the presence of a constant concentration of the other one.</description><subject>Aggregation number</subject><subject>Chemistry</subject><subject>Colloidal state and disperse state</subject><subject>Conductivity</subject><subject>Critical micelle concentration</subject><subject>Decyltrimethylammonium bromide</subject><subject>Exact sciences and technology</subject><subject>Fluorescence</subject><subject>General and physical chemistry</subject><subject>Hexadecyltrimethylammonium bromide</subject><subject>Ion-selective electrodes</subject><subject>Micelles. 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Thin films</topic><topic>Surface physical chemistry</topic><topic>Surface tension</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Rodríguez, J.L.</creatorcontrib><creatorcontrib>Sierra, M.B.</creatorcontrib><creatorcontrib>Messina, P.V.</creatorcontrib><creatorcontrib>Morini, M.A.</creatorcontrib><creatorcontrib>Schulz, P.C.</creatorcontrib><creatorcontrib>del Burgo, P.</creatorcontrib><creatorcontrib>Junquera, E.</creatorcontrib><creatorcontrib>Rodríguez, A.</creatorcontrib><creatorcontrib>Aicart, 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>Rodríguez, J.L.</au><au>Sierra, M.B.</au><au>Messina, P.V.</au><au>Morini, M.A.</au><au>Schulz, P.C.</au><au>del Burgo, P.</au><au>Junquera, E.</au><au>Rodríguez, A.</au><au>Aicart, E.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Surface and bulk properties of aqueous decyltrimethylammonium bromide–hexadecyltrimethylammonium bromide mixed system</atitle><jtitle>Journal of colloid and interface science</jtitle><addtitle>J Colloid Interface Sci</addtitle><date>2007-10-15</date><risdate>2007</risdate><volume>314</volume><issue>2</issue><spage>699</spage><epage>706</epage><pages>699-706</pages><issn>0021-9797</issn><eissn>1095-7103</eissn><coden>JCISA5</coden><abstract>The aqueous mixed system decyltrimethylammonium bromide (C 10TAB)–hexadecyltrimethylammonium bromide (C 16TAB) was studied by conductivity, ion-selective electrodes, surface tension, and fluorescence spectroscopy techniques. The mixture critical micelle concentration, cmc*, aggregation number, N ∗ , and micelle molar conductivity, Λ M cmc , showed that the system aggregation is strongly nonideal. Both cmc* and N ∗ results were analyzed with two different procedures: (i) the regular solution theory on mixed micelles or Rubingh's theory, and (ii) by the determination of the partial critical micelle concentration of the amphiphile component i in the presence of a constant concentration of the other amphiphile component, cmc i ∗ . The Rubingh procedure gives micelles richer in C 16TAB than the overall mixtures, while procedure (ii) gives micelles having the same composition as in the complete surfactant mixture ( α C 10 TAB ). Mixed micelles are larger than pure surfactant ones, with nonspherical shape. Using a literature model, the cause of the synergistic effect seems to be a reduction of the hydrocarbon/water contact at the micelle surface when mixed micelles form. Conductivity and ion-selective electrodes indicate that highly ionized premicelles form immediately before the cmc*. The air/solution interface is strongly nonideal and much richer in C 16 TAB than the composition in the bulk. When micelles form there is a strong desorption from the air/solution interface because micelles are energetically favored when compared with the monolayer. The aqueous mixed system C 10TAB–C 16TAB was studied by conductivity, ion-selective electrodes, surface tension, and fluorescence spectroscopy. Results were analyzed by the regular solution theory, and by the partial critical micelle concentration of one component in the presence of a constant concentration of the other one.</abstract><cop>San Diego, CA</cop><pub>Elsevier Inc</pub><pmid>17658541</pmid><doi>10.1016/j.jcis.2007.06.010</doi><tpages>8</tpages></addata></record>
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subjects Aggregation number
Chemistry
Colloidal state and disperse state
Conductivity
Critical micelle concentration
Decyltrimethylammonium bromide
Exact sciences and technology
Fluorescence
General and physical chemistry
Hexadecyltrimethylammonium bromide
Ion-selective electrodes
Micelles. Thin films
Surface physical chemistry
Surface tension
title Surface and bulk properties of aqueous decyltrimethylammonium bromide–hexadecyltrimethylammonium bromide mixed system
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