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An improved near- to far-zone transformation for the finite-difference time-domain method

机译:有限差分时域方法的一种改进的近到远区变换

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Near- to far-zone transformation for the finite-difference time-domain (FDTD) method can be performed by integration of the equivalent electric and magnetic currents originating from scattered electric and magnetic fields on a surface enclosing the object. Normally, when calculating the surface integrals, either the electric or magnetic fields are averaged since the electric and magnetic fields are spatially shifted in the FDTD grid. It is shown that this interpolation is unnecessary and also less accurate than if an integration is performed on two different surfaces. It is also shown that the accuracy of the far-zone transformation can be further improved if the phase is compensated with respect to a second-order dispersion corrected wavenumber. For validation, scattering results for an empty volume, a circular disk, and a sphere are compared with analytical solutions.
机译:有限差分时域(FDTD)方法的近到远区域转换可以通过将来自散射电场和磁场的等效电流和磁通电流积分到包围对象的表面上来执行。通常,在计算表面积分时,由于电场和磁场在FDTD网格中在空间上移动,因此对电场或磁场都进行了平均。结果表明,与在两个不同表面上进行积分相比,这种插值是不必要的,并且精度也较低。还显示出,如果相对于二阶色散校正的波数补偿相位,则可以进一步提高远区变换的精度。为了进行验证,将空体积,圆盘和球体的散射结果与分析溶液进行比较。

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