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DGTD Analysis of Electromagnetic Scattering from Penetrable Conductive Objects with IBC

机译:利用IBC的可穿透导电物体电磁散射的DGTD分析

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摘要

To avoid straightforward volumetric discretization, a discontinuous Galerkin time-domain (DGTD) method integrated with the impedance boundary condition (IBC) is presented in this paper to analyze the scattering from objects with finite conductivity. Two situations are considered: i) the skin depth is smaller than the thickness of the conductive volume; ii) the skin depth is larger than the thickness of a thin conductive sheet. For the first situation, a surface impedance boundary condition (SIBC) is employed, wherein the surface impedance usually exhibits a complex relation with the frequency. To incorporate the SIBC into DGTD, the surface impedance is firstly approximated by rational functions in the Laplace domain using the fast relaxation vector-fitting (FRVF) technique. Via inverse Laplace transform, the time-domain DGTD matrix equations can be obtained conveniently in integral form with respect to time t. For the second situation, a transmission IBC (TIBC) is used to include the transparent effects of the fields. In the TIBC, the tangential magnetic field jump is related with the tangential electric field via the surface conductivity. In this work, a specifically designed DGTD algorithm with TIBC is developed to model the graphene up to the terahertz (THz) band. In order to incorporate the TIBC into DGTD without involving the time-domain convolution, an auxiliary surface polarization current governed by a first order differential equation is introduced over the graphene. For open-region scattering problems, the DGTD algorithm is further hybridized with the time-domain boundary integral (TDBI) method to rigorously truncate the computational domain. To demonstrate the accuracy and applicability of the proposed algorithm, several representative examples are provided.
机译:为了避免直接的体积离散化,本文提出了一种与阻抗边界条件(IBC)集成的不连续Galerkin时域(DGTD)方法,以分析有限电导率物体的散射。考虑了两种情况:i)趋肤深度小于导电体积的厚度; ii)趋肤深度大于薄导电片的厚度。对于第一种情况,采用表面阻抗边界条件(SIBC),其中表面阻抗通常与频率呈复杂关系。为了将SIBC并入DGTD中,首先使用快速弛豫矢量拟合(FRVF)技术通过拉普拉斯域中的有理函数来近似表面阻抗。通过逆拉普拉斯逆变换,可以相对于时间t以积分形式方便地获得时域DGTD矩阵方程。对于第二种情况,使用传输IBC(TIBC)来包含字段的透明效果。在TIBC中,切向磁场跃变通过表面电导率与切向电场有关。在这项工作中,开发了一种专门设计的具有TIBC的DGTD算法,以对高达太赫兹(THz)频段的石墨烯进行建模。为了在不涉及时域卷积的情况下将TIBC合并到DGTD中,在石墨烯上引入了由一阶微分方程控制的辅助表面极化电流。对于开放区域散射问题,将DGTD算法与时域边界积分(TDBI)方法进一步混合,以严格截断计算域。为了证明所提出算法的准确性和适用性,提供了几个代表性的例子。

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