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Boundary element method solution of magnetohydrodynamic flow in a rectangular duct with conducting walls parallel to applied magnetic field

机译:导电壁平行于外加磁场的矩形管道中磁流体流动的边界元方法解

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The magnetohydrodynamic (MHD) flow of an incompressible, viscous, electrically conducting fluid in a rectangular duct with one conducting and one insulating pair of opposite walls under an external magnetic field parallel to the conducting walls, is investigated. The MHD equations are coupled in terms of velocity and magnetic field and cannot be decoupled with conducting wall boundary conditions since then boundary conditions are coupled and involve an unknown function. The boundary element method (BEM) is applied here by using a fundamental solution which enables to treat the MHD equations in coupled form with the most general form of wall conductivities. Also, with this fundamental solution it is possible to obtain BEM solution for values of Hartmann number (M) up to 300 which was not available before. The equivelocity and induced magnetic field contours which show the well-known characteristics of MHD duct flow are presented for several values of M.
机译:研究了矩形管道中不可压缩的粘性导电流体的磁流体动力学(MHD)流动,该矩形管道在平行于导电壁的外部磁场下具有一对导电壁和一对绝缘的相对壁。 MHD方程在速度和磁场方面是耦合的,不能与传导壁边界条件解耦,因为这样边界条件就耦合并包含未知函数。此处使用边界元法(BEM)通过使用一种基本解决方案,该解决方案能够以耦合形式与最一般形式的壁电导率来处理MHD方程。同样,利用这种基本解决方案,可以获得哈特曼数(M)高达300的BEM解决方案,而这是以前无法获得的。对于M的几个值,给出了等速和感应磁场轮廓,这些轮廓显示了MHD管道流的众所周知的特性。

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