We'll follow [1,2] and references therein (ref's to be completed) to implement the FE approximation of incompressible resistive MHD equations. As a first step we will focus on low Re & Ha numbers to avoid introducing stabilization terms. We'll follow [1] to implement mixed FE.
Following the formulation in [1], the discrete problem reads: find
and
such that for any
and
it holds
where
.
Discretizing above equations with implicit Euler results in exact satisfaction of the Gauss low for every time step, this follows from [Thm 1, 1]. In [Sect. 3.4, 1] explicit Picard and Newton formulations can be found.
Tasks
References
[1] K. Hu, Y. Ma & J. Xu Stable Finite Element Methods Preserving ∇ · B = 0 Exactly for MHD Models Numerische Mathematik, 135, 371–396 (2017)
[2] R. Planas STABILIZED FINITE ELEMENT FORMULATIONS FOR SOLVING INCOMPRESSIBLE
MAGNETOHYDRODYNAMICS PhD Thesis (2013)
We'll follow [1,2] and references therein (ref's to be completed) to implement the FE approximation of incompressible resistive MHD equations. As a first step we will focus on low Re & Ha numbers to avoid introducing stabilization terms. We'll follow [1] to implement mixed FE.
Following the formulation in [1], the discrete problem reads: find
and
such that for any
and
it holds
where
.
Discretizing above equations with implicit Euler results in exact satisfaction of the Gauss low for every time step, this follows from [Thm 1, 1]. In [Sect. 3.4, 1] explicit Picard and Newton formulations can be found.
Tasks
References
[1] K. Hu, Y. Ma & J. Xu Stable Finite Element Methods Preserving ∇ · B = 0 Exactly for MHD Models Numerische Mathematik, 135, 371–396 (2017)
[2] R. Planas STABILIZED FINITE ELEMENT FORMULATIONS FOR SOLVING INCOMPRESSIBLE
MAGNETOHYDRODYNAMICS PhD Thesis (2013)