Departmental Papers (MEAM)

Document Type

Journal Article

Date of this Version

September 2002

Comments

Copyright (2002) American Institute of Physics. This article may be downloaded for personal use only. Any other use requires prior permission of the author and the American Institute of Physics. Reprinted from Physics of Fluids, Volume 14, Issue 10, September 2002, pages 3584-3592.
Publisher URL: http://dx.doi.org/10.1063/1.1504713

Abstract

Magnetohydrodynamics may potentially provide a convenient means for controlling fluid flow and stirring fluids in minute fluidic networks. The branches of such fluidic networks consist of conduits with rectangular cross sections. Each conduit has two individually controlled electrodes positioned along opposing walls and additional disk-shaped electrodes deposited in the conduit's interior away from its sidewalls. The network is positioned in a uniform magnetic field. When one applies a potential difference between a disk-shaped electrode and two wall electrodes acting in tandem, circulatory motion is induced in the conduit. When the potential difference alternates periodically across two or more such configurations, complicated (chaotic) motions evolve. As the period of alternation increases, so does the complexity of the flow. We derive a two-dimensional, time-independent expression for the magnetohydrodynamic creeping flow around a centrally positioned disk-shaped electrode in the limit of zero radius. With the aid of this expression, the trajectories of passive tracers are computed as functions of the alternations protocol and the electrodes' locations. The theoretical results are qualitatively compared with flow visualization experiments.

Keywords

magnetohydrodynamics, rotational flow, flow control, microfluidics, chaos, creeping flow, flow visualisation

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Date Posted: 22 October 2007

This document has been peer reviewed.