The DRBEM solution of Cauchy MHD duct flow with a slipping and variably conducting wall using the well-posed iterations

Cemre Aydin, M. Tezer-Sezgin
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Abstract

The present study focuses on the numerical investigation of the Cauchy Magnetohyrodynamic (MHD) duct flow in the presence of an externally applied oblique magnetic field, with a slipping and variably conducting wall portion of the duct walls. The underspecified and overspecified boundary informations for the velocity of the fluid and the induced magnetic field on both slipping and variably conducting duct wall and its opposite part, respectively, constitutes the Cauchy MHD duct flow problem. This study aims to recompute the velocity of the fluid and induced magnetic field with specified slip length and conductivity constant, respectively, on the underspecified wall which is both slipping and variably conducting. The governing coupled convection-diffusion type MHD equations for the direct and inverse formulations are solved in one stroke using the dual reciprocity boundary element method (DRBEM). Both the velocity and induced magnetic field and their normal derivatives to be used as overspecified boundary conditions for the construction of Cauchy problem are obtained through the direct formulation of the problem. The well-posed iterations are used in the regularization of the ill-conditioned systems of linear algebraic equations resulting from the DRBEM discretization of Cauchy problem (inverse problem). Numerical solutions for the slip velocity and induced magnetic field are obtained for Hartmann number values $M$=5, 10, 50. The main advantages of the DRBEM are its boundary only nature and the capability of providing both the unknowns and their normal derivatives on the underspecified walls so that the conductivity constant and the slip length between them can be recovered at a low computational expense.
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采用适定迭代法求解具有滑动变导壁的柯西MHD管道流动的DRBEM
本文主要研究了柯西磁流体动力学(MHD)管道在外加斜磁场作用下的流动,以及管道壁面滑动和变传导壁面部分的数值研究。流体速度的边界信息不明确和边界信息过明确构成了柯西MHD风道流动问题。本研究旨在重新计算指定滑移长度和电导率常数的流体速度和感应磁场在指定既滑移又变导电的壁面上的速度。采用对偶互易边界元法(DRBEM)一次求解了正、逆耦合对流扩散型MHD控制方程。通过对柯西问题的直接表述,得到了速度和感应磁场及其法向导数作为构造柯西问题的过规定性边界条件。利用良定迭代对柯西问题(反问题)的DRBEM离散化所产生的病态线性代数方程组进行正则化。得到了哈特曼数$M$= 5,10,50时滑移速度和感应磁场的数值解。DRBEM的主要优点是其仅限边界的特性,以及能够在未指定的壁面上提供未知量及其法向导数,从而可以以较低的计算成本恢复它们之间的电导率常数和滑移长度。
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来源期刊
CiteScore
3.30
自引率
6.20%
发文量
13
审稿时长
16 weeks
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