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Solution of time domain electric field integral equation for arbitrarily shaped dielectric bodies using an unconditionally stable methodology

机译:使用无条件稳定方法求解任意形状介电体的时域电场积分方程

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In this work, we present a new and efficient numerical method to obtain an unconditionally stable solution for the time domain electric field integral equation (TD-EFIE) for arbitrary homogeneous dielectric bodies, derived utilizing the surface equivalence principle. This novel method does not utilize the customary marching-on in time solution method often used to solve a hyperbolic partial differential equation. Instead we solve the wave equation by expressing the transient behaviors in terms of weighted Laguerre polynomials. By using these orthonormal basis functions for the temporal variation, the time derivatives in the TD-EFIE formulation can be handled analytically. Since these weighted Laguerre polynomials converge to zero as time progresses, the induced electric and magnetic currents when expanded in a series of weighted Laguerre polynomials also converge to zero. In order to solve the wave equation, we introduce two separate testing procedures, a spatial and temporal testing. By introducing first the temporal testing procedure, the marching-on in time procedure is replaced by a recursive relation between the different orders of the weighted Laguerre polynomials. The other novelty of this approach is that through the use of the entire domain Laguerre polynomials for the expansion of the temporal variation of the currents, the spatial and the temporal variables can be separated. For convenience, we use the Hertz vector as the unknown variable instead of the equivalent electric current density. However, we use the equivalent magnetic current density as it is. To verify our method, we apply the proposed method to various dielectric scatterers and compare the results of an inverse Fourier transform of a frequency domain EFIE.
机译:在这项工作中,我们提出了一种新的高效数值方法,它利用表面等效原理推导了任意均质介电体的时域电场积分方程(TD-EFIE)的无条件稳定解。这种新颖的方法没有利用通常用于求解双曲型偏微分方程的惯常行进时间解法。相反,我们通过用加权Laguerre多项式表示瞬态行为来求解波动方程。通过将这些正交函数用于时间变化,可以解析地处理TD-EFIE公式中的时间导数。由于这些加权的Laguerre多项式随着时间的流逝而收敛于零,因此在一系列加权的Laguerre多项式中展开时的感应电流和磁流也收敛于零。为了求解波动方程,我们引入了两个单独的测试过程,即空间和时间测试。通过首先引入时间测试过程,在时间上进行的过程被加权拉盖尔多项式的不同阶之间的递归关系所代替。这种方法的另一个新颖之处在于,通过使用整个域Laguerre多项式来扩展电流的时间变化,可以将空间和时间变量分开。为方便起见,我们使用赫兹向量作为未知变量,而不是等效电流密度。但是,我们按原样使用等效磁电流密度。为了验证我们的方法,我们将提出的方法应用于各种介质散射体,并比较了频域EFIE的傅立叶逆变换的结果。

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