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Error Analysis of a PFEM Based on the Euler Semi-Implicit Scheme for the Unsteady MHD Equations

In this article, we mainly consider a first order penalty finite element method (PFEM) for the 2D/3D unsteady incompressible magnetohydrodynamic (MHD) equations. The penalty method applies a penalty term to relax the constraint “ [Formula: see text] ”, which allows us to transform the saddle point p...

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Detalles Bibliográficos
Autores principales: Shi, Kaiwen, Su, Haiyan, Feng, Xinlong
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9602181/
https://www.ncbi.nlm.nih.gov/pubmed/37420415
http://dx.doi.org/10.3390/e24101395
Descripción
Sumario:In this article, we mainly consider a first order penalty finite element method (PFEM) for the 2D/3D unsteady incompressible magnetohydrodynamic (MHD) equations. The penalty method applies a penalty term to relax the constraint “ [Formula: see text] ”, which allows us to transform the saddle point problem into two smaller problems to solve. The Euler semi-implicit scheme is based on a first order backward difference formula for time discretization and semi-implicit treatments for nonlinear terms. It is worth mentioning that the error estimates of the fully discrete PFEM are rigorously derived, which depend on the penalty parameter [Formula: see text] , the time-step size [Formula: see text] , and the mesh size h. Finally, two numerical tests show that our scheme is effective.