PSTD算法:一种快速、准确的电子封装表征时域方法

Q. Liu, Y. Li, J. Liao
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引用次数: 1

摘要

传统的时域有限差分(FDTD)方法在模拟大规模复杂介质中的电磁波传播时效率很低。这主要是由于时域有限差分法中空间离散化的精度较低。因此,即使对于中等大小的问题,也需要大量的细胞(通常每个波长10-20个细胞)才能获得相当准确的结果。对于大规模问题,由于色散误差随着传播距离的增加而迅速增大,这一要求变得更加严格。近年来,人们提出了一种伪谱时域(PSTD)算法,无论问题大小如何,每个波长只需要两个单元。在空间离散化方面,该方法是一种最优的时域解,因为它在空间表示上具有无限阶的精度。对于比最小波长小得多的结构问题,PSTD算法仍然具有比FDTD方法高得多的空间频率精度。此外,PSTD算法中引入的唯一误差是时间离散化。与FDTD方法中的色散误差不同,该误差是各向同性的,并且不随问题的规模而增加。在这项工作中,我们应用PSTD方法来表征电子封装的电气性能。特别地,它被用来研究外壳共振和电磁干扰的影响。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
The PSTD algorithm: a fast and accurate time-domain method for electronic package characterization
Conventional finite-difference time-domain (FDTD) methods are very inefficient for simulations of electromagnetic wave propagation in large-scale complex media. This is mainly because of the low-accuracy associated with the spatial discretization in the FDTD methods. As a result, even for a moderate size problem, a large number of cells (typically 10-20 cells per wavelength) are required to obtain reasonably accurate results. This requirement becomes much more stringent for large-scale problems since the dispersion error grows rapidly with the propagation distance. Recently a pseudospectral time-domain (PSTD) algorithm has been developed which requires only two cells per wavelength regardless of the problem size. In terms of spatial discretization, this method is an optimal time-domain solution since it has an infinite order of accuracy in the spatial representation. For a problem with structures much smaller than the smallest wavelength, the PSTD algorithm still provides high accuracy up to a much higher spatial frequency than FDTD methods. In addition, the only error introduced in the PSTD algorithm is the temporal discretization. Unlike the dispersion error in FDTD methods, this error is isotropic and does not increase with the scale of the problem. In this work, we apply the PSTD method to characterize the electrical performance of electronic packages. In particular, it is used to investigate the effects of enclosure resonance and electromagnetic interference.
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