Boundary layer near the surface of a solid body and low-frequency dielectric dispersion

S. Dukhin
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引用次数: 5

Abstract

The paper deals with the possibility of studying the stagnant part of the boundary layer on the basis of effects due to polarization of the electrochemical double layer (DL). A theory is developed for polarization of the diffuse part of a thin DL of a spherical particle in a direct and alternating field, allowing for the effect of ion flow through the stagnant part of the DL. Formulae are obtained on the basis of this theory for electrophoresis complicated by polarization and for the large low-frequency dielectric dispersion (ω). Calculation of the stagnant layer thickness and the ionic mobilities of this layer is shown to be possible on the basis of electrophoretic measurement on three fractions of spherical particles with identical values of ψd and ζ. Using only one fraction, we can obtain similar information from the low-frequency section of (ω).
靠近固体表面的边界层和低频介电色散
本文在电化学双层极化效应的基础上,探讨了研究边界层停滞部分的可能性。提出了一种理论,用于在直接和交变场中球形颗粒的薄DL的扩散部分的极化,允许离子流通过DL的停滞部分的影响。在此理论的基础上,得到了极化复杂电泳和大低频介电色散(ω)的计算公式。在对具有相同的ψd和ζ值的三种球形粒子进行电泳测量的基础上,可以计算停滞层的厚度和该层的离子迁移率。仅使用一个分数,我们就可以从(ω)的低频部分获得类似的信息。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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