A linearity preserving nodal variation limiting algorithm for continuous Galerkin discretization of ideal MHD equations

• Published in: Journal of computational physics Vol. 410; no. C; p. 109390
• Main Authors: Mabuza, Sibusiso, Shadid, John N., Cyr, Eric C., Pawlowski, Roger P., Kuzmin, Dmitri
• Format: Journal Article
• Language: English
• Published: Cambridge Elsevier Inc 01-06-2020; Elsevier Science Ltd; Elsevier
• Subjects: Algebraic flux correction; Algorithms; Artificial diffusion; Compressibility; Computational fluid dynamics; Computational physics; Constraining; Continuous Galerkin methods; Discretization; Divergence; Galerkin method; Hyperbolic systems; Iterative limiters; Iterative methods; Linearity; Linearity preservation; Lumping; Magnetohydrodynamics; Mathematical analysis; Stabilization; Time integration; Iterative limiters; Linearity preservation; Artificial diffusion; Magnetohydrodynamics; Algebraic flux correction; Continuous Galerkin methods
• ISSN: 0021-9991; 1090-2716
• DOI: 10.1016/j.jcp.2020.109390

•A new continuous finite element method for inviscid ideal MHD systems is presented.•Algebraic flux correction based on monolithic nodal variation limiting.•Linearity preserving limiting for MHD systems.•Demonstration of flexible and robust implicit and explicit time integrators.
In this work, a stabilized continuous Galerkin (CG) method for magnetohydrodynamics (MHD) is presented. Ideal, compressible inviscid MHD equations are discretized in space on unstructured meshes using piecewise linear or bilinear finite element bases to get a semi-discrete scheme. Stabilization is then introduced to the semi-discrete method in a strategy that follows the algebraic flux correction paradigm. This involves adding some artificial diffusion to the high order, semi-discrete method and mass lumping in the time derivative term. The result is a low order method that provides local extremum diminishing properties for hyperbolic systems. The difference between the low order method and the high order method is scaled element-wise using a limiter and added to the low order scheme. The limiter is solution dependent and computed via an iterative linearity preserving nodal variation limiting strategy. The stabilization also involves an optional consistent background high order dissipation that reduces phase errors. The resulting stabilized scheme is a semi-discrete method that can be applied to inviscid shock MHD problems and may be even extended to resistive and viscous MHD problems. To satisfy the divergence free constraint of the MHD equations, we add parabolic divergence cleaning to the system. Various time integration methods can be used to discretize the scheme in time. We demonstrate the robustness of the scheme by solving several shock MHD problems.