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Comparison of the GHS_(Smooth) and the Rayleigh-Rice surface scatter theories

机译:GHS_(平滑)和Rayleigh-Rice表面散射理论的比较

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The scalar-based GHS_(Smooth) surface scatter theory results in an expression for the BRDF in terms of the surface PSD that is very similar to that provided by the rigorous Rayleigh-Rice (RR) vector perturbation theory. However it contains correction factors for two extreme situations not shared by the RR theory: (ⅰ) large incident or scattered angles that result in some portion of the scattered radiance distribution falling outside of the unit circle in direction cosine space, and (ⅱ) the situation where the relevant rms surface roughness, σ_(rel), is less than the total intrinsic rms roughness of the scattering surface. Also, the RR obliquity factor has been discovered to be an approximation of the more general GHS_(Smooth) obliquity factor due to a little-known (or long-forgotten) implicit assumption in the RR theory that the surface autocovariance length is longer than the wavelength of the scattered radiation. This assumption allowed retaining only quadratic terms and lower in the series expansion for the cosine function, and results in reducing the validity of RR predictions for scattering angles greater than 60°. This inaccurate obliquity factor in the RR theory is also the cause of a complementary unrealistic "hook" at the high spatial frequency end of the predicted surface PSD when performing the inverse scattering problem. Furthermore, if we empirically substitute the polarization reflectance, Q, from the RR expression for the scalar reflectance, R, in the GHS_(Smooth) expression, it inherits all of the polarization capabilities of the rigorous RR vector perturbation theory.
机译:基于标量的GHS_(Smooth)表面散射理论可得出BRDF的表面PSD表达式,该表达式与严格的Rayleigh-Rice(RR)矢量扰动理论所提供的表达式非常相似。但是,它包含了RR理论未共享的两种极端情况的校正因子:(ⅰ)大入射角或散射角,导致散射辐射分布的某些部分落在方向余弦方向上的单位圆之外,并且(ⅱ)相关的均方根表面粗糙度σ_(rel)小于散射表面的总固有均方根粗糙度的情况。同样,由于RR理论中一个鲜为人知(或长期被遗忘的)隐含假设,即表面自协方差长度长于GHS_(平滑)倾斜因数,因此RR倾斜因数是更一般的GHS_(平滑)倾斜因数的近似值。散射辐射的波长。该假设仅保留二次项,而余弦函数的级数展开较低,并且导致散射角度大于60°的RR预测的有效性降低。 RR理论中的这种不正确的倾斜因子也是在执行逆散射问题时在预测表面PSD的高空间频率端出现互补的不现实“钩子”的原因。此外,如果我们根据经验将RR表达式中的偏振反射率Q替换为GHS_(Smooth)表达式中的标量反射率R,则它将继承严格的RR矢量摄动理论的所有偏振能力。

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