BEM solution to magnetohydrodynamic flow in a semi-infinite?duct

被引:3
|
作者
Bozkaya, Canan [1 ]
Tezer-Sezgin, M. [1 ]
机构
[1] Middle E Tech Univ, Dept Math, TR-06531 Ankara, Turkey
关键词
MHD; BEM; semi-infinite region; BOUNDARY-ELEMENT METHOD; TRANSVERSE MAGNETIC-FIELD; HIGH HARTMANN NUMBERS; FINITE-ELEMENT; DUCT FLOW; MHD FLOW; RECTANGULAR DUCT; WALL CONDUCTIVITY; EQUATIONS; PARALLEL;
D O I
10.1002/fld.2689
中图分类号
TP39 [计算机的应用];
学科分类号
081203 ; 0835 ;
摘要
We consider the magnetohydrodynamic flow that is laminar and steady of a viscous, incompressible, and electrically conducting fluid in a semi-infinite duct under an externally applied magnetic field. The flow is driven by the current produced by a pressure gradient. The applied magnetic field is perpendicular to the semi-infinite walls that are kept at the same magnetic field value in magnitude but opposite in sign. The wall that connects the two semi-infinite walls is partly non-conducting and partly conducting (in the middle). A BEM solution was obtained using a fundamental solution that enables to treat the magnetohydrodynamic equations in coupled form with general wall conductivities. The inhomogeneity in the equations due to the pressure gradient was tackled, obtaining a particular solution, and the BEM was applied with a fundamental solution of coupled homogeneous convectiondiffusion type partial differential equations. Constant elements were used for the discretization of the boundaries (y ?=? 0, -a ? x ? a) and semi-infinite walls at x ?=? +/- a, by keeping them as finite since the boundary integral equations are restricted to these boundaries due to the regularity conditions as y ????8?. The solution is presented in terms of equivelocity and induced magnetic field contours for several values of Hartmann number (M), conducting length (l), and non-conducting wall conditions (k). The effect of the parameters on the solution is studied. Flow rates are also calculated for these values of parameters. Copyright (C) 2011 John Wiley & Sons, Ltd.
引用
收藏
页码:300 / 312
页数:13
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