Transient rotating electromagnetohydrodynamic micropumps between two infinite microparallel plates

被引:41
|
作者
Jian, Yongjun [1 ]
Si, Dongqing [1 ]
Chang, Long [2 ]
Liu, Quansheng [1 ]
机构
[1] Inner Mongolia Univ, Sch Math Sci, Hohhot 010021, Inner Mongolia, Peoples R China
[2] Inner Mongolia Univ Finance & Econ, Sch Math & Stat, Hohhot 010051, Inner Mongolia, Peoples R China
基金
中国国家自然科学基金;
关键词
Electromagnetohydrodynamic (EMHD); Micropump; Hartmann number; Rotating Reynolds number; Method of separation of variables; POWER-LAW FLUIDS; ELECTROOSMOTIC FLOW; MAXWELL FLUIDS; MHD MICROPUMP; TRANSPORT; ELEMENT; CHANNEL;
D O I
10.1016/j.ces.2015.04.036
中图分类号
TQ [化学工业];
学科分类号
0817 ;
摘要
By using the method of separation of variables, analytical investigations are performed for combined transient rotating electromagnetohydrodynamic (EMHD) flow of an electrically conducting, incompressible and viscous fluid between two slit microparallel plates. The flow relies on the rotating effect and the Lorentz force produced by the interaction between an externally imposed electrical current and a transverse magnetic field. Three different cases associated with electric and magnetic fields are discussed respectively, i.e., uniform electric and magnetic fields (case I); AC electric field and uniform magnetic field (case II); AC electric and magnetic fields (case III). The variations of velocity profiles and volume flow rates with time and their dependence on the rotating Reynolds number Rea and the Hartmann number Ha are explained graphically. The results show that the magnitude of rotating EMHD velocity increases with Ha within a range when Ha <3 in our present analysis. With the increase of the rotating Reynolds number, the magnitude of rotating EMHD velocity decreases in axial direction and increases in lateral direction. For small rotating Reynolds number Rea, an interesting phenomenon for case I is that the maximum is not shifted and the maximum of the velocity in axial direction is the minimum of the velocity in lateral direction, and vice versa. However, there is a shift of the maximum for large rotating Reynolds number Rea. Under the case II and the case III, the periodic oscillating phenomenon of the rotating EMHD velocity occurs. In addition, for three cases, the flow rate in y* direction increases with Hartmann number and decreases with rotating Reynolds number. The amplitude of EMHD velocity is larger under the case II than that of steady solution under case I, but smaller than that under case III for prescribed Hartmann number Ha and rotating Reynolds number Rea. Interestingly, there is a giant augmentation of the flow rates both in axial and in lateral directions for case III due to the aiding part of Lorentz force being greatly larger than retarding one in certain parameter ranges of phase of the magnetic field relative to the electrical field. By comparing our theoretical results in the limit case without rotation effect with related experimental data, the analytical results coincide qualitatively with the fitted curve obtained in experiments. (C) 2015 Elsevier Ltd. All rights reserved.
引用
收藏
页码:12 / 22
页数:11
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