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首页> 外文期刊>Computational Mechanics: Solids, Fluids, Fracture Transport Phenomena and Variational Methods >A meshfree weak-strong (MWS) form method for the unsteady magnetohydrodynamic (MHD) flow in pipe with arbitrary wall conductivity
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A meshfree weak-strong (MWS) form method for the unsteady magnetohydrodynamic (MHD) flow in pipe with arbitrary wall conductivity

机译:任意壁电导率的管道中不稳定磁流体动力学(MHD)流的无网格弱强(MWS)形成方法

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In this paper a meshfree weak-strong (MWS) form method is considered to solve the coupled equations in velocity and magnetic field for the unsteady magnetohydrodynamic flow throFor this modified estimaFor this modified estimaFor this modified estimaugh a pipe of rectangular and circular sections having arbitrary conducting walls. Computations have been performed for various Hartman numbers and wall conductivity at different time levels. The MWS method is based on applying a meshfree collocation method in strong form for interior nodes and nodes on the essential boundaries and a meshless local Petrov-Galerkin method in weak form for nodes on the natural boundary of the domain. In this paper, we employ the moving least square reproducing kernel particle approximation to construct the shape functions. The numerical results for sample problems compare very well with steady state solution and other numerical methods.
机译:本文考虑采用无网格弱强(MWS)形式的方法来求解非恒定磁流体动力流在速度和磁场中的耦合方程式。墙壁。已经在不同的时间水平对各种哈特曼数和壁电导率进行了计算。 MWS方法基于对内部节点和本质边界上的节点应用强形式的无网格搭配方法,对域的自然边界上的节点应用弱形式的无网格局部Petrov-Galerkin方法。在本文中,我们采用移动最小二乘再现核粒子逼近来构造形状函数。样本问题的数值结果与稳态解和其他数值方法相比非常好。

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