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Numerical calculation of diffraction coefficients of genericconducting and dielectric wedges using FDTD

机译:用FDTD数值计算通用导体和介质楔的衍射系数

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摘要

Classical theories such as the uniform geometrical theory of diffraction (UTD) utilize analytical expressions for diffraction coefficient for canonical problems such as the infinite perfectly conducting wedge. We present a numerical approach to this problem using the finite-difference time-domain (FDTD) method. We present results for the diffraction coefficient of the two-dimensional (2-D) infinite perfect electrical conductor (PEC) wedge, the 2-D infinite lossless dielectric wedge, and the 2-D infinite lossy dielectric wedge for incident TM and TE polarization and a 90° wedge angle. We compare our FDTD results in the far-field region for the infinite PEC wedge to the well-known analytical solutions obtained using the UTD. There is very good agreement between the FDTD and UTD results. The power of this approach using FDTD goes well beyond the simple problems dealt with in this paper. It can, in principle, be extended to calculate the diffraction coefficients for a variety of shape and material discontinuities, even in three dimensions
机译:诸如统一的衍射几何理论(UTD)之类的经典理论利用诸如无穷完美导电楔的典型问题的衍射系数解析表达式。我们提出了一种使用时域有限差分(FDTD)方法解决此问题的数值方法。我们给出了二维(2-D)无限完美电导体(PEC)楔,2-D无限无损介电楔和2-D无限有损介电楔对入射TM和TE极化的衍射系数的结果和90°楔角。我们将无限远PEC楔的远场区域中的FDTD结果与使用UTD获得的著名分析解决方案进行比较。 FDTD和UTD结果之间有很好的一致性。使用FDTD的这种方法的功能远远超出了本文所讨论的简单问题。原则上,它可以扩展为计算各种形状和材料不连续性的衍射系数,即使在三个维度上

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