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绝缘壁附近倾斜金属纳米线的感应电荷电泳

Induced-charge electrophoresis of a tilted metal nanowire near an insulating wall.

作者信息

Flores-Mena Jose Eladio, García-Sánchez Pablo, Ramos Antonio

机构信息

Facultad de Ciencias de la Electrónica, Benemérita Universidad Autónoma de Puebla, Av. San Claudio y 18 Sur, San Manuel, CU. FCE2, 72570 Puebla, Mexico.

Departamento de Electrónica y Electromagnetismo, Facultad de Física, Universidad de Sevilla, Avda. Reina Mercedes s/n, 41012 Sevilla, Spain.

出版信息

Phys Rev E. 2024 Apr;109(4-2):045109. doi: 10.1103/PhysRevE.109.045109.

DOI:10.1103/PhysRevE.109.045109
PMID:38755876
Abstract

Electric fields are commonly used to control the orientation and motion of microscopic metal particles in aqueous suspensions. For example, metallodielectric Janus spheres are propelled by the induced-charge electro-osmotic flow occurring on their metallic side, the most common case in electrokinetics of exploiting symmetry breaking of surface properties for achieving net particle motion. In this work, we demonstrate that a homogeneous metal rod can translate parallel to a dielectric wall as a result of the hydrodynamic wall-particle interaction arising from the induced-charge electro-osmosis on the rod surface. The applied electric field could be either dc or low-frequency ac. The only requirement for a nonvanishing particle velocity is that the axis of the rod be inclined with respect to the wall, i.e., it cannot be neither parallel nor perpendicular. We show numerical results of the rod velocity as a function of rod orientation and distance to the wall. The maximum particle velocity is found for an orientation of between ∼30^{∘} and ∼50^{∘}, depending on the position and aspect ratio of the cylinder. Particle velocities of up to tens of µm/s are predicted for typical conditions in electrokinetic experiments.

摘要

电场通常用于控制水悬浮液中微观金属颗粒的取向和运动。例如,金属电介质双面球由其金属面上发生的感应电荷电渗流推动,这是电动学中利用表面性质对称性破缺实现颗粒净运动的最常见情况。在这项工作中,我们证明,由于棒表面感应电荷电渗作用产生的流体动力壁 - 颗粒相互作用,一根均匀的金属棒可以平行于电介质壁平移。施加的电场可以是直流或低频交流。颗粒速度不为零的唯一要求是棒的轴相对于壁倾斜,即它既不能平行也不能垂直。我们展示了棒速度作为棒取向和到壁距离的函数的数值结果。根据圆柱体的位置和纵横比,在约30°至约50°的取向之间发现了最大颗粒速度。对于电动实验中的典型条件,预测颗粒速度可达数十微米/秒。

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