2018
DOI: 10.1090/mcom/3341
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Structure-preserving finite element methods for stationary MHD models

Abstract: In this paper, we develop a class of mixed finite element scheme for stationary magnetohydrodynamics (MHD) models, using magnetic field B and current density j as the discretization variables. We show that the Gauss's law for the magnetic field, namely ∇·B = 0, and the energy law for the entire system are exactly preserved in the finite element schemes. Based on some new basic estimates for H h (div), we show that the new finite element scheme is well-posed. Furthermore, we show the existence of solutions to t… Show more

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Cited by 38 publications
(37 citation statements)
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“…We also show another strategy to impose the strong divergence-free condition, instead of using Lagrange multipliers as in the previous work [21] by one of the authors and collaborator. We introduce an augmented term (∇ · B, ∇ · C) in the variational formulation.…”
Section: Introductionmentioning
confidence: 98%
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“…We also show another strategy to impose the strong divergence-free condition, instead of using Lagrange multipliers as in the previous work [21] by one of the authors and collaborator. We introduce an augmented term (∇ · B, ∇ · C) in the variational formulation.…”
Section: Introductionmentioning
confidence: 98%
“…To preserve magnetic Gauss's law precisely on the discrete level with electric and magnetic fields as variables, a class of finite element schemes was developed in [20,21] for the time dependent and the stationary MHD systems respectively. The magnetic field B is discretized by the H(div) conforming Raviart-Tomas [27] or BDM [9] elements.…”
Section: Introductionmentioning
confidence: 99%
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