On the Maxwell-wave equation coupling problem and its explicit finite-element solution

Pub Date : 2022-06-22 DOI:10.21136/AM.2022.0210-21
Larisa Beilina, Vitoriano Ruas
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引用次数: 3

Abstract

It is well known that in the case of constant dielectric permittivity and magnetic permeability, the electric field solving the Maxwell’s equations is also a solution to the wave equation. The converse is also true under certain conditions. Here we study an intermediate situation in which the magnetic permeability is constant and a region with variable dielectric permittivity is surrounded by a region with a constant one, in which the unknown field satisfies the wave equation. In this case, such a field will be the solution of Maxwell’s equation in the whole domain, as long as proper conditions are prescribed on its boundary. We show that an explicit finite-element scheme can be used to solve the resulting Maxwell-wave equation coupling problem in an inexpensive and reliable way. Optimal convergence in natural norms under reasonable assumptions holds for such a scheme, which is certified by numerical exemplification.

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麦克斯韦波动方程耦合问题及其显式有限元解
众所周知,在介电常数和磁导率恒定的情况下,求解麦克斯韦方程组的电场也是波动方程的解。在某些条件下,反之亦然。在这里,我们研究了一种中间情况,其中磁导率是常数,具有可变介电常数的区域被具有常数的区域包围,其中未知场满足波动方程。在这种情况下,只要在其边界上规定了适当的条件,这样的场将是麦克斯韦方程在整个域中的解。我们证明,显式有限元格式可以用一种廉价可靠的方法来解决由此产生的麦克斯韦波动方程耦合问题。在合理假设下,自然范数的最优收敛性适用于这样的方案,并通过数值例子证明了这一点。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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