Title of article
High-order conservative finite difference GLM–MHD schemes for cell-centered MHD
Author/Authors
Mignone، نويسنده , , Andrea and Tzeferacos، نويسنده , , Petros and Bodo، نويسنده , , Gianluigi، نويسنده ,
Issue Information
روزنامه با شماره پیاپی سال 2010
Pages
25
From page
5896
To page
5920
Abstract
We present and compare third- as well as fifth-order accurate finite difference schemes for the numerical solution of the compressible ideal MHD equations in multiple spatial dimensions. The selected methods lean on four different reconstruction techniques based on recently improved versions of the weighted essentially non-oscillatory (WENO) schemes, monotonicity preserving (MP) schemes as well as slope-limited polynomial reconstruction. The proposed numerical methods are highly accurate in smooth regions of the flow, avoid loss of accuracy in proximity of smooth extrema and provide sharp non-oscillatory transitions at discontinuities.
gest a numerical formulation based on a cell-centered approach where all of the primary flow variables are discretized at the zone center. The divergence-free condition is enforced by augmenting the MHD equations with a generalized Lagrange multiplier yielding a mixed hyperbolic/parabolic correction, as in Dedner et al. [J. Comput. Phys. 175 (2002) 645–673]. The resulting family of schemes is robust, cost-effective and straightforward to implement. Compared to previous existing approaches, it completely avoids the CPU intensive workload associated with an elliptic divergence cleaning step and the additional complexities required by staggered mesh algorithms.
ive numerical testing demonstrate the robustness and reliability of the proposed framework for computations involving both smooth and discontinuous features.
Keywords
Higher-order methods , WENO schemes , Monotonicity preserving , Cell-centered methods , Magnetohydrodynamics , compressible flow
Journal title
Journal of Computational Physics
Serial Year
2010
Journal title
Journal of Computational Physics
Record number
1482505
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