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Discretization of the electric-magnetic field integral equation with the divergence Taylor-Orthogonal basis functions free from the magnetic-field and the electric-field low-frequency breakdowns

机译:电磁场积分方程的离散化与发散泰勒 - 正交基函数没有磁场和电场低频故障

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The discretization of the Electric-Magnetic Field Integral Equation (EMFIE) with the divergence Taylor-Orthogonal basis functions (div-TO) mitigates the observed discrepancy in the computed RCS for sharp-edged objects of the RWG-discretization of the Magnetic-Field Integral Equation (MFIE) with respect to the Electric-Field Integral Equation (EFIE). The EMFIE is derived from the application of the normal-electric and the tangential-magnetic boundary conditions at the surface of the body. The div-TO discretization of the EMFIE in the very low frequency regime shows huge inaccuracies in the computed RCS due to breakdowns arising from both the magnetic-field and the electric-field contributions. In this paper, we present an implementation of the EMFIE with the div-TO basis functions free from these failures in the low frequency regime.
机译:具有发散泰勒 - 正交基函数(DIV-To)的电磁场积分方程(EMFIE)的离散化减轻了计算RCS中的观察到的差异,用于磁场积分的RWG离散化的尖锐边缘对象 等式(MFIE)关于电场积分方程(EFIE)。 EMFIE源自普通电动和体之间的施加在体内的施加。 由于磁场和电场贡献产生的故障,所计算的RCS在非常低频状态下,EMFIE的DIV-离散化表现出巨大的不准确性。 在本文中,我们在低频制度中展示了emfie的实施,没有这些失败。

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