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Theoretical and computational aspects of scattering from rough surfaces: one-dimensional perfectly reflecting surfaces

机译:从粗糙表面散射的理论和计算方面:一维完美反射的表面

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We discuss the scattering of acoustic or electromagnetic waves from one-dimensional rough surfaces. We restrict the discussion in this report to perfectly reflecting Dirichlet surfaces (TE polarization). The theoretical development is for both infinite and periodic surfaces, the latter equations being derived from the former. We include both derivations for completeness of notation. Several theoretical developments are presented. They are characterized by integral equation solutions for the surface current or normal derivative of the total field. All the equations are discretized to a matrix system and further characterized by the sampling of the rows and columns of the matrix which is accomplished in either coordinate space (C) or spectral space (S). The standard equations are referred to here as CC equations of either the first (CC1) or second kind (CC2). Mixed representation, or SC-type, equations are solved as well as SS equations fully in spectral space. Computational results are presented for scattering from various periodic surfaces. The results include examples with grazing incidence, a very rough surface and a highly oscillatory surface. The examples vary over a parameter set which includes the geometrical optics regime, physical optics or resonance regime, and a renormalization regime. The objective of this study was to determine the best computational method for these problems. Briefly, the SC method was the fastest, but it did not converge for large slopes or very rough surfaces for reasons we explain. The SS method was slower and had the same convergence difficulties as SC. The CC methods were extremely slow but always converged. The simplest approach is to try the SC method first. Convergence, when the method works, is very fast. If convergence does not occur with SC, then SS should be used, and failing that CC. [References: 19]
机译:我们讨论一维粗糙表面对声波或电磁波的散射。我们将本报告中的讨论限制为完美地反映Dirichlet表面(TE极化)。理论上的发展是针对无限和周期性表面,后者是从前者推导出来的。我们包括两种表示法完整性的推导。介绍了一些理论发展。它们的特征是表面电流或整个场的正态导数的积分方程解。将所有方程式离散化为矩阵系统,并进一步以在坐标空间(C)或光谱空间(S)中完成的矩阵行和列的采样为特征。标准方程式在这里称为第一类(CC1)或第二类(CC2)的CC方程式。混合表示或SC型方程以及SS方程都在光谱空间中求解。给出了从各种周期性表面散射的计算结果。结果包括具有掠入射,非常粗糙的表面和高度振荡的表面的示例。这些示例在包括几何光学方案,物理光学或共振方案以及重归一化方案的参数集上变化。这项研究的目的是为这些问题确定最佳的计算方法。简而言之,SC方法是最快的方法,但是由于我们解释的原因,它在大坡度或非常粗糙的表面上没有收敛。 SS方法较慢,并且具有与SC相同的收敛困难。 CC方法非常慢,但始终会收敛。最简单的方法是先尝试使用SC方法。该方法可行时,收敛速度非常快。如果SC不会发生收敛,则应使用SS,并使CC失败。 [参考:19]

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