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Meshless local boundary integral equation (LBIE) method for the unsteady magnetohydrodynamic (MHD) flow in rectangular and circular pipes

机译:矩形和圆形管道中非定常磁流体动力学(MHD)流动的无网格局部边界积分方程(LBIE)方法

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The meshless local boundary integral equation (LBIE) method is given to obtain the numerical solution of the coupled equations in velocity and magnetic field for unsteady magnetohydrodynamic (MHD) flow through a pipe of rectangular and circular sections with non-conducting walls. Computations have been carried out for different Hartmann numbers and at various time levels. The method is based on the local boundary integral equation with moving least squares (MLS) approximation. For the MLS, nodal points spread over the analyzed domain, are utilized to approximate the interior and boundary variables. A time stepping method is employed to deal with the time derivative. Finally, numerical results are presented to show the behaviour of velocity and induced magnetic field.
机译:给出了无网格局部边界积分方程(LBIE)的方法,以得到非定常磁流体动力学(MHD)流经矩形和圆形截面非导电壁管的速度和磁场耦合方程的数值解。已经针对不同的哈特曼数和在不同的时间水平上进行了计算。该方法基于具有移动最小二乘(MLS)近似的局部边界积分方程。对于MLS,利用在分析域中分布的节点来近似内部和边界变量。采用时间步进方法来处理时间导数。最后,数值结果表明了速度和感应磁场的行为。

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