On stabilized P1 finite element approximation fortime harmonic Maxwell's equations
M. Asadzadeh, L. Beilina

TL;DR
This paper develops and analyzes a stabilized finite element method for time harmonic Maxwell's equations, transforming the hyperbolic problem into an elliptic form to ensure stability, convergence, and robustness of the numerical scheme.
Contribution
It introduces a stabilized linear finite element approach for Maxwell's equations in dual form, providing theoretical convergence proofs and adaptive algorithms validated by numerical experiments.
Findings
Proves coercivity and unique solvability of the stabilized scheme.
Establishes optimal convergence rates of O(h) in L2 and residual norms.
Validates robustness through numerical examples.
Abstract
One way of improving the behavior of finite element schemes for classical, time-dependent Maxwell's equations, is to render them from their hyperbolic character to elliptic form. This paper is devoted to the study of the stabilized linear finite element method for the time harmonic Maxwell's equations in a dual form obtained through the Laplace transformation in time. The model problem is for the particular case of the dielectric permittivity function which is assumed to be constant in a boundary neighborhood. For the stabilized model a coercivity relation is derived that guarantee's the existence of a unique solution for the iscrete problem. The convergence is addressed both in a priori and a posteriori settings. In the a priori error estimates we confirm the theoretical convergence of the scheme in a L2-based, gradient dependent, triple norm. The order of convergence is O(h) in…
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Taxonomy
TopicsAdvanced Numerical Methods in Computational Mathematics · Electromagnetic Simulation and Numerical Methods · Numerical methods in engineering
