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.

Highlights

  • The effects of magnetic field through the electrically conducting fluids, such as electrolytes, blood plasmas, salt waters, liquid metals etc. are concerned by the magnetohyrodynamics (MHD)

  • When the direct problem is solved for a specified slip length and conductivity constant with Dirichlet type velocity and induced magnetic field conditions, the opposite side of the duct wall contains overspecified conditions

  • The direct and Cauchy formulations are constructed for the MHD rectangular duct flow problems in terms of the slip velocity and induced magnetic field on the left wall, and they are solved by using the dual reciprocity boundary element method (DRBEM)

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Summary

Introduction

The effects of magnetic field through the electrically conducting fluids, such as electrolytes, blood plasmas, salt waters, liquid metals etc. are concerned by the magnetohyrodynamics (MHD). Slip length and conductivity constant on these parts of the boundary can be determined when the MHD flow problem is designed as a Cauchy problem In this case, the boundary conditions for the velocity of the fluid can be incomplete either in the form of underspecified or overspecified on different parts of the boundary. The slip length and the conductivity constant are assumed to be unknown in the inverse or Cauchy problem and both the velocity, the induced magnetic field and their normal derivatives are going to be determined which are underspecified boundary conditions on that part of the duct walls. When the direct problem is solved for a specified slip length and conductivity constant with Dirichlet type velocity and induced magnetic field conditions, the opposite side of the duct wall contains overspecified conditions (both the velocity, induced magnetic field and their normal derivatives obtained from the direct DRBEM solution). It enables us to obtain the solution of Cauchy MHD flow problem at a small computational expense

Mathematical formulation of the problem
The DRBEM application
The well-posed iterations
Numerical results
Reconstruction of the slip length and the conductivity constant
Findings
Conclusion slip length conductivity constant
Full Text
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