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非离子型胶束与癸烷水溶液中的多组分扩散

Multicomponent Diffusion in Aqueous Solutions of Nonionic Micelles and Decane.

作者信息

Alexander Nathan P, Phillips Ronald J, Dungan Stephanie R

出版信息

Langmuir. 2019 Oct 22;35(42):13595-13606. doi: 10.1021/acs.langmuir.9b01823. Epub 2019 Oct 10.

DOI:10.1021/acs.langmuir.9b01823
PMID:31553616
Abstract

Taylor dispersion and dynamic light scattering techniques were used to measure the ternary diffusivity matrix [] and the micelle gradient diffusion coefficient, respectively, in crowded aqueous solutions of decaethylene glycol monododecyl ether (CE) and decane. The results indicate that CE diffused down its own gradient with the micelle gradient diffusivity while decane diffused down a decane gradient at a much slower rate. Furthermore, strong diffusion coupling, comprising decane diffusion down a surfactant gradient and surfactant diffusion up a decane gradient, was also observed with cross diffusivities that were on the order of or larger than the main diffusivities. Measurements of the micelle aggregation number, hydration index, and the hydrodynamic radius, obtained using both static and dynamic light scattering methods, indicate that decane-containing micelles interacted as hard spheres and had radii and aggregation numbers that increased linearly with the molar ratio of solute to surfactant. A theoretical model, developed using Batchelor's theory for gradient diffusion in a polydisperse system of interacting hard spheres, was effectively used to predict [] with no adjustable parameters. A comparison with the theory indicates that decane diffused down its own gradient by micelle -diffusion while surfactant diffused down a surfactant gradient by micelle diffusion. It is also shown that intermicellar interactions drove decane diffusion down a CE gradient by a volume exclusion effect while an increase in the micelle aggregation number and hydrodynamic radius with decane was necessary to drive surfactant diffusion up a decane gradient.

摘要

采用泰勒分散法和动态光散射技术,分别测量了十甘醇单十二烷基醚(CE)和癸烷的拥挤水溶液中的三元扩散率矩阵[]和胶束梯度扩散系数。结果表明,CE以胶束梯度扩散率沿自身梯度扩散,而癸烷沿癸烷梯度扩散的速度要慢得多。此外,还观察到了强烈的扩散耦合,包括癸烷沿表面活性剂梯度扩散和表面活性剂沿癸烷梯度向上扩散,其交叉扩散率与主要扩散率相当或更大。使用静态和动态光散射方法测得的胶束聚集数、水合指数和流体动力学半径表明,含癸烷的胶束表现为硬球相互作用,其半径和聚集数随溶质与表面活性剂的摩尔比线性增加。利用Batchelor理论建立的多分散相互作用硬球系统中梯度扩散的理论模型,在无可调参数的情况下有效地预测了[]。与理论的比较表明,癸烷通过胶束扩散沿自身梯度扩散,而表面活性剂通过胶束扩散沿表面活性剂梯度扩散。研究还表明,胶束间相互作用通过体积排除效应驱动癸烷沿CE梯度扩散,而胶束聚集数和流体动力学半径随癸烷的增加是驱动表面活性剂沿癸烷梯度向上扩散的必要条件。

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