Chiu Han C, Keh Huan J
Department of Chemical Engineering, National Taiwan University, Taipei, Taiwan.
Electrophoresis. 2017 Oct;38(19):2468-2478. doi: 10.1002/elps.201700074. Epub 2017 May 12.
The diffusiophoresis of a charged sphere along the axis of a circular microtube filled with an electrolyte solution is studied theoretically. The tube wall may be either nonconductive and impermeable or prescribed with a linear electrolyte concentration distribution. The electric double layers at the solid surfaces are thin, but the diffuse-layer polarization effect over the particle surface is considered. The general solutions to the electrokinetic differential equations are expressed in spherical and cylindrical coordinates, whereas the boundary conditions at the particle surface are satisfied by a collocation technique. The collocation solutions for the diffusiophoretic velocity of the particle, which are in good agreement with the asymptotic formula derived from a reflection method, are obtained for various values of the radius ratio and zeta potential ratio between the particle and the microtube and of other relevant parameters. The contributions from the diffusioosmotic flow along the tube wall and wall-corrected diffusiophoretic driving force to the particle velocity can be superimposed due to the linearity. Although the diffusiophoretic velocity in an uncharged microtube is in general a decreasing function of the particle-to-tube radius ratio and can reverse its direction, it can increase with increases in this ratio due to the competition of the wall effects of possible electrochemical enhancement and hydrodynamic retardation to the particle motion. When the zeta potentials associated with the tube and particle are equivalent, the diffusioosmotic flow induced by the tube wall dominates the diffusiophoretic motion.
从理论上研究了带电球体在充满电解质溶液的圆形微管轴线上的扩散电泳。管壁可以是不导电且不可渗透的,或者规定有线性电解质浓度分布。固体表面的双电层很薄,但考虑了颗粒表面的扩散层极化效应。电动微分方程的通解用球坐标和柱坐标表示,而颗粒表面的边界条件通过配置技术来满足。对于颗粒与微管之间的半径比、zeta电位比以及其他相关参数的各种值,获得了与通过反射方法导出的渐近公式高度一致的颗粒扩散电泳速度的配置解。由于线性关系,沿管壁的扩散渗透流和壁面校正的扩散电泳驱动力对颗粒速度的贡献可以叠加。尽管在不带电微管中的扩散电泳速度通常是颗粒与管半径比的递减函数,并且可以反转其方向,但由于可能的电化学增强和流体动力学阻滞对颗粒运动的壁面效应的竞争,它可以随着该比值的增加而增加。当与管和颗粒相关的zeta电位相等时,由管壁引起的扩散渗透流主导扩散电泳运动。