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Plane waves in FDTD simulations and a nearly perfect total-field/scattered-field boundary

机译:FDTD模拟中的平面波和近乎完美的全场/散场边界

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The total-field/scattered-field (TFSF) boundary has been successfully used for a number of years to introduce energy into finite-difference time-domain (FDTD) grids. If the propagation of the incident field is grid-aligned, a perfect TFSF implementation can be realized by using an auxiliary one-dimensional FDTD simulation which models propagation of the incident field. Here "perfect" implies the incident field propagation exactly matches the way in which the field propagates in the FDTD grid. However, for propagation which is not grid-aligned, no similarly perfect implementation has previously been presented. This work provides a framework for a perfect TFSF boundary for pulsed plane waves which do not propagate in a grid-aligned fashion. To achieve this, homogeneous plane-wave propagation is rigorously quantified. Using this knowledge and a specification of the desired incident field, the dispersion relation is used to ascertain the incident field at any point in the grid. It is required to account for, unlike in the continuous world, the electric field, the magnetic field, and the wavenumber vector not forming a mutually orthogonal set. Group velocity is also considered because of its relevance to the implementation.
机译:总场/散射场(TFSF)边界已经成功使用了很多年,以将能量引入有限差分时域(FDTD)网格。如果入射场的传播是网格对齐的,则可以通过使用辅助一维FDTD仿真(对入射场的传播进行建模)来实现完美的TFSF实现。此处,“完美”表示入射场传播与FDTD网格中场传播的方式完全匹配。但是,对于没有网格对齐的传播,以前没有提出过类似的完美实现。这项工作为脉冲平面波的完美TFSF边界提供了一个框架,该脉冲不会以网格对齐的方式传播。为此,严格地对均匀的平面波传播进行量化。利用这些知识和所需入射场的规范,可以使用色散关系来确定网格中任意点处的入射场。与连续世界不同,需要考虑电场,磁场和波数矢量不形成相互正交的集合。还考虑了组速度,因为它与实现相关。

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