The classical treatments of the primary electroviscous effect show important discrepancies with respect to the experimental data. A possible better agreement may be found if the contribution of the ions adsorbed on the Stern layer, which can move tangentially near the particle surface, is taken into
The Primary Electroviscous Effect: Thin Double Layers (aκ⪢1) and a Stern Layer
✍ Scribed by J.D. Sherwood; F.J. Rubio-Hernández; E. Ruiz-Reina
- Publisher
- Elsevier Science
- Year
- 2000
- Tongue
- English
- Weight
- 86 KB
- Volume
- 228
- Category
- Article
- ISSN
- 0021-9797
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✦ Synopsis
The primary electroviscous effect due to the charge clouds surrounding spherical charged particles suspended in an electrolyte was studied by Hinch and Sherwood (J. Fluid Mech. 132, 337 (1983)) in the limit of double layers thin compared to the particle radius a. Here we introduce the effect of a dynamic Stern layer into that analysis, in order to explain the numerical results of Rubio-Hernández et al. (J. Colloid Interface Sci. 206, 334 (1998)) in terms of the ratio of the tangential ionic fluxes within the charge cloud to those within the Stern layer. The predictions of the asymptotic analysis are compared with those of numerical computations. The thickness of the charge cloud is characterized by the Debye length kappa(-1). If akappa>10 the predictions of the asymptotic analysis exhibit the same qualitative behavior as the numerical results, but akappa>1000 is required to achieve quantitative agreement to within 2.5%. Copyright 2000 Academic Press.
📜 SIMILAR VOLUMES
The theory developed by Watterson and White (Watterson, I. G., and White, L. R., J. Chem. Soc., Faraday Trans. 2 77, 1115 (1981)) to calculate the primary electroviscous coefficient of a suspension of charged spherical colloidal particles has been extended, by considering the presence of a dynamic S