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Singular boundary method for 3D time-harmonic electromagnetic scattering problems

机译:3D时谐电磁散射问题的奇异边界法

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A frequency domain singular boundary method is presented for solving 3D time-harmonic electromagnetic scattering problem from perfect electric conductors. To avoid solving the coupled partial differential equations with fundamental solutions involving hypersingular terms, we decompose the governing equation into a system of independent Helmholtz equations with mutually coupled boundary conditions. Then the singular boundary method employs the fundamental solutions of the Helmholtz equations to approximate the scattered electric field variables. To desingularize the source singularity in the fundamental solutions, the origin intensity factors are introduced. In the novel formulation, only the origin intensity factors for fundamental solutions of 3D Helmholtz equations and its derivatives need to be considered which have been derived in the paper. Several numerical examples involving various perfectly conducting obstacles are carried out to demonstrate the validity and accuracy of the present method. (C) 2019 Elsevier Inc. All rights reserved.
机译:提出了一种频域奇异边界方法,用于求解理想导体的3D时谐电磁散射问题。为了避免使用涉及超奇异项的基本解来求解耦合的偏微分方程,我们将控制方程分解为具有相互耦合的边界条件的独立亥姆霍兹方程组。然后,奇异边界方法利用Helmholtz方程的基本解来近似散射电场变量。为了在基本解中对源奇点进行奇化处理,引入了原点强度因子。在新的公式中,仅需考虑3D Helmholtz方程及其衍生物的基本解的原点强度因子,这些原点强度因子已在本文中得出。进行了涉及多个完美传导障碍的几个数值示例,以证明本方法的有效性和准确性。 (C)2019 Elsevier Inc.保留所有权利。

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