Zhao Hui
Department of Mechanical Engineering, University of Nevada, Las Vegas, Nevada 89154, USA.
Phys Rev E Stat Nonlin Soft Matter Phys. 2010 Jun;81(6 Pt 2):066314. doi: 10.1103/PhysRevE.81.066314. Epub 2010 Jun 23.
Bubbles can be trapped inside textured structures such as grooves, forming a superhydrophobic surface. A superhydrophobic surface has a large effective hydrodynamic slip length compared to a smooth hydrophobic surface and holds the promise of enhancing electrokinetic flows that find many interesting applications in microfluidics. However, recent theoretical studies suggested that electro-osmotic flows over a weakly charged superhydrophobic surface [the zeta potential of the surface is smaller than the thermal potential (25 mV)] can only be enhanced when liquid-gas interfaces are charged [T. M. Squires, Phys. Fluids 20, 092105 (2008); Bahga, J. Fluid Mech. 644, 245 (2010)]. So far there is little work reported when the zeta potential of the surface is comparable or even larger than the thermal potential. In this paper we numerically investigate electro-osmotic flows over a periodically striped slip-stick surface by solving the standard Poisson-Nernst-Planck equations. Our results indicate that at large zeta potentials, even if liquid-gas interfaces are charged, the nonuniform surface conduction due to the mismatch between surface conductions over no-shear and no-slip regions leads to electric field lines penetrating the double layer and thus the nonuniform surface conduction weakens the tangential component of the electric field which primarily drives electro-osmotic flows. Our results imply that, in the presence of strong nonuniform surface conduction, enhanced electro-osmotic flows over a superhydrophobic surface are possible only in certain conditions. In particular, the enhancement due to the slip can potentially be lost at large zeta potentials. Similar loss of the enhancement of a charged particle's electrophoretic mobility due to the slip was reported by Khair and Squires [Phys. Fluids 21, 042001 (2009)].
气泡可能被困在诸如凹槽等有纹理的结构内部,从而形成超疏水表面。与光滑疏水表面相比,超疏水表面具有较大的有效流体动力学滑移长度,并有望增强电动流动,而电动流动在微流体中有许多有趣的应用。然而,最近的理论研究表明,在弱带电超疏水表面上的电渗流(表面的zeta电位小于热电位(25 mV))只有在液 - 气界面带电时才能增强 [T. M. Squires, Phys. Fluids 20, 092105 (2008); Bahga, J. Fluid Mech. 644, 245 (2010)]。到目前为止,当表面的zeta电位与热电位相当甚至更大时,几乎没有相关工作报道。在本文中,我们通过求解标准的泊松 - 能斯特 - 普朗克方程,对周期性条纹状滑移 - 黏附表面上的电渗流进行了数值研究。我们的结果表明,在大zeta电位下,即使液 - 气界面带电,由于无剪切和无滑移区域表面传导不匹配导致的非均匀表面传导会使电场线穿透双层,从而非均匀表面传导削弱了主要驱动电渗流的电场切向分量。我们的结果意味着,在存在强非均匀表面传导的情况下,超疏水表面上增强的电渗流仅在特定条件下才可能实现。特别是,在大zeta电位下,由于滑移导致的增强可能会丧失。Khair和Squires [Phys. Fluids 21, 042001 (2009)] 报道了由于滑移导致带电粒子电泳迁移率增强的类似丧失情况。