Simultaneous Observation of Attractive Interaction, Depletion Forces, and “Sticky” Encounters between AOT Reverse Micelles in Isooctane Using Microelectrode Voltammetry
Microelectrode voltammetry has been used to measure the long-time self-diffusion coefficients (D s) of AOT (AOT = sodium bis-2-ethylhexylsulfosuccinate) reverse micelles in isooctane using K3Fe(CN)6 as a micelle-immobilized electroactive probe. D s values were found to be a function of both reverse...
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Veröffentlicht in: | The journal of physical chemistry. B 2000-08, Vol.104 (33), p.8061-8067 |
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description | Microelectrode voltammetry has been used to measure the long-time self-diffusion coefficients (D s) of AOT (AOT = sodium bis-2-ethylhexylsulfosuccinate) reverse micelles in isooctane using K3Fe(CN)6 as a micelle-immobilized electroactive probe. D s values were found to be a function of both reverse micellar volume fraction (φ mic) and probe concentration. The results show that increasing the probe concentration results in a decrease in D s, suggesting an increase in attractive intermicellar interaction upon addition of probe. This has been interpreted in terms of attenuated surfactant tail-group reorganization facilitating interpenetrating of the surfactant tails. Increasing the micellar volume fraction is seen to diminish attractive interaction which indicates the presence of entropy-driven solvent mediated depletion forces. Self-diffusion coefficients at the limit of zero probe concentration ( ) were found to be micellar volume fraction dependent, and the behavior conformed to the linear interaction theory for interacting micellar systems giving an attractive intermicellar interaction parameter of −2.33. Extrapolation to infinite dilution (i.e., φ mic → 0, the limit of zero interaction) reveals a reverse micellar long-time self-diffusion coefficient ( ) of 6.13 ± 0.07 × 10-7 cm-2 s-1, which gives a corresponding micellar hydrodynamic radius of 7.5 ± 0.02 nm. This value is approximately a factor of 2 greater than the know micellar size, and the behavior is interpreted in terms of adhesive “sticky” intermicellar interactions indicating the measurements of micellar cluster diffusion. |
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D s values were found to be a function of both reverse micellar volume fraction (φ mic) and probe concentration. The results show that increasing the probe concentration results in a decrease in D s, suggesting an increase in attractive intermicellar interaction upon addition of probe. This has been interpreted in terms of attenuated surfactant tail-group reorganization facilitating interpenetrating of the surfactant tails. Increasing the micellar volume fraction is seen to diminish attractive interaction which indicates the presence of entropy-driven solvent mediated depletion forces. Self-diffusion coefficients at the limit of zero probe concentration ( ) were found to be micellar volume fraction dependent, and the behavior conformed to the linear interaction theory for interacting micellar systems giving an attractive intermicellar interaction parameter of −2.33. Extrapolation to infinite dilution (i.e., φ mic → 0, the limit of zero interaction) reveals a reverse micellar long-time self-diffusion coefficient ( ) of 6.13 ± 0.07 × 10-7 cm-2 s-1, which gives a corresponding micellar hydrodynamic radius of 7.5 ± 0.02 nm. This value is approximately a factor of 2 greater than the know micellar size, and the behavior is interpreted in terms of adhesive “sticky” intermicellar interactions indicating the measurements of micellar cluster diffusion.</description><identifier>ISSN: 1520-6106</identifier><identifier>EISSN: 1520-5207</identifier><identifier>DOI: 10.1021/jp9923015</identifier><language>eng</language><publisher>American Chemical Society</publisher><ispartof>The journal of physical chemistry. 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Self-diffusion coefficients at the limit of zero probe concentration ( ) were found to be micellar volume fraction dependent, and the behavior conformed to the linear interaction theory for interacting micellar systems giving an attractive intermicellar interaction parameter of −2.33. Extrapolation to infinite dilution (i.e., φ mic → 0, the limit of zero interaction) reveals a reverse micellar long-time self-diffusion coefficient ( ) of 6.13 ± 0.07 × 10-7 cm-2 s-1, which gives a corresponding micellar hydrodynamic radius of 7.5 ± 0.02 nm. 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B</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Charlton, Ian D</au><au>Doherty, Andrew P</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Simultaneous Observation of Attractive Interaction, Depletion Forces, and “Sticky” Encounters between AOT Reverse Micelles in Isooctane Using Microelectrode Voltammetry</atitle><jtitle>The journal of physical chemistry. B</jtitle><addtitle>J. Phys. Chem. B</addtitle><date>2000-08-24</date><risdate>2000</risdate><volume>104</volume><issue>33</issue><spage>8061</spage><epage>8067</epage><pages>8061-8067</pages><issn>1520-6106</issn><eissn>1520-5207</eissn><abstract>Microelectrode voltammetry has been used to measure the long-time self-diffusion coefficients (D s) of AOT (AOT = sodium bis-2-ethylhexylsulfosuccinate) reverse micelles in isooctane using K3Fe(CN)6 as a micelle-immobilized electroactive probe. D s values were found to be a function of both reverse micellar volume fraction (φ mic) and probe concentration. The results show that increasing the probe concentration results in a decrease in D s, suggesting an increase in attractive intermicellar interaction upon addition of probe. This has been interpreted in terms of attenuated surfactant tail-group reorganization facilitating interpenetrating of the surfactant tails. Increasing the micellar volume fraction is seen to diminish attractive interaction which indicates the presence of entropy-driven solvent mediated depletion forces. Self-diffusion coefficients at the limit of zero probe concentration ( ) were found to be micellar volume fraction dependent, and the behavior conformed to the linear interaction theory for interacting micellar systems giving an attractive intermicellar interaction parameter of −2.33. Extrapolation to infinite dilution (i.e., φ mic → 0, the limit of zero interaction) reveals a reverse micellar long-time self-diffusion coefficient ( ) of 6.13 ± 0.07 × 10-7 cm-2 s-1, which gives a corresponding micellar hydrodynamic radius of 7.5 ± 0.02 nm. This value is approximately a factor of 2 greater than the know micellar size, and the behavior is interpreted in terms of adhesive “sticky” intermicellar interactions indicating the measurements of micellar cluster diffusion.</abstract><pub>American Chemical Society</pub><doi>10.1021/jp9923015</doi><tpages>7</tpages></addata></record> |
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title | Simultaneous Observation of Attractive Interaction, Depletion Forces, and “Sticky” Encounters between AOT Reverse Micelles in Isooctane Using Microelectrode Voltammetry |
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