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EDGE ELEMENT METHODS FOR MAXWELL'S EQUATIONS WITH STRONG CONVERGENCE FOR GAUSS' LAWS

机译:高斯定律强收敛的麦克斯韦方程组的边缘元素方法

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摘要

In this paper we propose and investigate some edge element approximations for three Maxwell systems in three dimensions: the stationary Maxwell equations, the time-harmonic Maxwell equations, and the time-dependent Maxwell equations. These approximations have three novel features. First, the resulting discrete edge element systems can be solved by some existing preconditioned solvers with optimal convergence rate independent of finite element meshes, including the stationary Maxwell equations. Second, they ensure the optimal strong convergence of Gauss' laws in some appropriate norm, in addition to the standard optimal convergence in energy norm, under the general weak regularity assumptions that hold for both convex and nonconvex polyhedral domains and for the discontinuous coefficients that may have large jumps across the interfaces between different media. Finally, no saddle-point discrete systems are needed to solve for the stationary Maxwell equations, unlike most existing edge element schemes.
机译:在本文中,我们提出并研究了三个Maxwell系统在三个维度上的一些边元近似:平稳Maxwell方程,时谐Maxwell方程和与时间相关的Maxwell方程。这些近似具有三个新颖的特征。首先,可以通过一些现有的预处理求解器以最佳收敛速度求解所得离散边缘单元系统,而最优收敛速度与有限元网格无关,包括平稳的麦克斯韦方程组。其次,除了在能量规范上的标准最佳收敛之外,它们还确保了高斯定律在某些适当的范本中的最佳强收敛,这适用于对凸和非凸多面体域以及不连续系数可能适用的一般弱规律性假设。在不同媒体之间的接口上有很大的跳跃。最后,与大多数现有的边缘单元方案不同,不需要鞍点离散系统来求解平稳的麦克斯韦方程。

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