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Convolution-Free Modelling of Dispersive Media in the Time-Domain Finite-Element Solution of the Vector Wave Equation

机译:矢量波方程时域有限元解的无分散媒体的无卷积建模

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A new approach to derive finite-element time-domain (FETD) formulations for modelling a general linear dispersive media is developed. The formulation starts from the mixed FETD discretized by Whitney forms in space and the Crank-Nicolson (CN) method in time. The effect of the media dispersion is taken into account separately using a bilinear transformation approach. Having combined these equations, a formulation is reached that reduces to the second-order vector wave equation discretized by the Newmark-β method with β = 1/4 in non-dispersive media. So, our formulation can be considered as an extension of the unconditionally stable (US) vector wave equation to dispersive media using a bilinear transformation method. Therefore, it does not suffer from intrinsic limitations of the existing convolution-based formulations. Furthermore, it can be concluded that the CN-FETD is a mixed version of the vector wave equation discretized by Whitney forms in space and the US Newmark-β method in time. Finally, the formulation is applied to obtain reflection and transmission coefficients of a doubly dispersive dielectric slab and highly accurate results are reached.
机译:开发了一种推导有限元时间域(FETD)制剂的新方法是开发用于建模一般线性分散介质的制剂。该配方从惠特尼离散化的混合的FETD在空间和曲柄 - 尼古尔森(CN)方法中开始。使用双线性转换方法分别考虑介质分散的效果。结合了这些等式,达到了一种制剂,其减少到由非分散介质中的β= 1/4的纽马克-β方法离散的二阶矢量波方程。因此,我们的配方可以被认为是使用双线性变换方法的无条件稳定(US)矢量波方程的延伸,以分散介质。因此,它不会遭受现有的基于卷积的制剂的内在限制。此外,可以得出结论,CN-FETD是通过惠特尼在空间和美国纽马克-β方法中被惠特尼形式离散的矢量波方程的混合版本。最后,施加制剂以获得双层分散介电板的反射和透射系数,并且达到高精度结果。

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