FHD flow in an irregular cavity subjected to a non-uniform magnetic field

P. Senel
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Abstract

In this paper FHD flow in a rectangular pipe constricted by two analogous semi-cylinders attached to the left and the bottom walls is investigated. The laminar, axial flow is produced by a constant pressure gradient, and the flow is affected by a spatially varying non-uniform magnetic field caused by two electric wires. The current-carrying wires are placed along the axes of the semi-cylinders. The fully developed flow is studied on the 2D cross-section of the pipe, a cavity, where the wires act as point magnetic sources. The pressure equation is added to the mathematical model, and the velocity-pressure form governing equations are numerically solved by the dual reciprocity boundary element method (DRBEM). The Dirichlet type pressure boundary conditions are approximated through a process using the radial basis functions and a finite difference. The flow, velocity, and pressure variations are investigated for different magnetic field strengths and current ratios. The grid independence study is also carried out. The proposed iterative scheme is capable of generating numerical results by performing a non-uniform discretization for the boundary. Dense discretizations are applied at the places where the flow shows a sudden fluctuation. It is shown by the numerical results that the flow and the pressure variations are dominated by the strong magnetic source. With an increment in the magnetic number, the planar flow is accelerated, the axial flow is decelerated, and the pressure increases, especially around the strong point magnetic source.
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在非均匀磁场作用下,FHD在不规则腔体中的流动
本文研究了矩形管中的FHD流动,矩形管由连接在左壁和底壁上的两个类似的半圆柱体约束。层流轴向流动是由恒定的压力梯度产生的,并且流动受到由两根电线引起的空间变化的不均匀磁场的影响。载流导线沿着半圆柱体的轴线放置。在管道的二维横截面上研究了完全发展的流动,管道是一个空腔,其中导线充当点磁源。在数学模型中加入了压力方程,并采用对偶互易边界元法对速度-压力形式的控制方程进行了数值求解。通过使用径向基函数和有限差分的过程来近似狄利克雷型压力边界条件。研究了不同磁场强度和电流比下的流量、速度和压力变化。还进行了网格独立性研究。所提出的迭代方案能够通过对边界执行非均匀离散化来生成数值结果。在流量出现突然波动的地方应用密集离散化。数值结果表明,强磁源对流体的流动和压力变化起主导作用。随着磁数的增加,平面流加速,轴向流减速,压力增加,尤其是在强点磁源周围。
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