Hsu Jyh-Ping, Hsu Wei-Lun, Chen Zheng-Syun
Department of Chemical Engineering; National Taiwan University, Taipei, Taiwan 10617.
Langmuir. 2009 Feb 3;25(3):1772-84. doi: 10.1021/la803334a.
The boundary effect on the diffusiophoretic behavior of a particle is analyzed theoretically by considering the diffusiophoresis of a charged sphere under arbitrary surface potential and double-layer thickness at an arbitrary position in an uncharged spherical cavity. We show that the phenomenon under consideration is governed by double-layer relaxation, chemiosmotic/diffusioosmotic flow, and two types of competing double-layer polarization. The presence of the cavity has a profound influence on the diffusiophoretic behavior of the particle, especially when the surface potential is high. For instance, the scaled diffusiophoretic velocity of the particle has a local maximum as the position of the particle varies; it may have a local maximum and local minimum as the thickness of the double-layer varies. The significance of the effect of double-layer relaxation depends upon the level of surface potential and magnitude of the electric Peclet number.
通过考虑在无电荷球形腔内任意位置处,具有任意表面电势和双层厚度的带电球体的扩散泳动,从理论上分析了边界对粒子扩散泳动行为的影响。我们表明,所考虑的现象由双层弛豫、化学渗透/扩散渗透流以及两种竞争的双层极化所控制。腔体的存在对粒子的扩散泳动行为有深远影响,特别是当表面电势较高时。例如,随着粒子位置的变化,粒子的标度化扩散泳动速度会出现局部最大值;随着双层厚度的变化,它可能会出现局部最大值和局部最小值。双层弛豫效应的重要性取决于表面电势的水平和电佩克莱数的大小。