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A robust finite element method for incompressible magnetohydrodynamics using Whitney forms
Abstract
A stabilized semi-discrete finite element scheme for the incompressible magnetohydrodynamics system is presented. The scheme uses the Whitney $2$-form and $1$-form for the fluid velocity and magnetic induction, respectively. The key ingredient is a magnetic curl-jump penalty term, which allows us to prove a pre-asymptotic error estimate of order O(h1/2) with a constant depending on solution norms but not explicitly on the fluid viscosity and magnetic diffusivity.
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BibTeX
@misc{yu2026robust,
title = {{A robust finite element method for incompressible magnetohydrodynamics using Whitney forms}},
author = {Tianwei Yu},
howpublished = {arXiv},
year = {2026},
month = oct,
doi = {10.48550/arxiv.2610.26606},
eprint = {2610.26606},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2610.26606},
}
RIS
TY - UNPB
TI - A robust finite element method for incompressible magnetohydrodynamics using Whitney forms
AU - Tianwei Yu
PY - 2026
DA - 2026/10/19
PB - arXiv
DO - 10.48550/arxiv.2610.26606
UR - https://arxiv.org/abs/2610.26606
AB - A stabilized semi-discrete finite element scheme for the incompressible magnetohydrodynamics system is presented. The scheme uses the Whitney $2$-form and $1$-form for the fluid velocity and magnetic induction, respectively. The key ingredient is a magnetic curl-jump penalty term, which allows us to prove a pre-asymptotic error estimate of order O(h^1/2) with a constant depending on solution norms but not explicitly on the fluid viscosity and magnetic diffusivity.
ER -