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首页> 外文期刊>Applied optics >SCATTERING OF LIGHT BY POLYDISPERSE, RANDOMLY ORIENTED, FINITE CIRCULAR CYLINDERS
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SCATTERING OF LIGHT BY POLYDISPERSE, RANDOMLY ORIENTED, FINITE CIRCULAR CYLINDERS

机译:多分散,有限定向的有限圆柱体对光的散射

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We use the T-matrix method, as described by Mishchenko [Appl. Opt. 32, 4652 (1993)], to compute rigorously light scattering by finite circular cylinders in random orientation. First we discuss numerical aspects of T-matrix computations specific for finite cylinders and present results of benchmark computations for a simple cylinder model. Then we report results of extensive computations for polydisperse, randomly oriented cylinders with a refractive index of 1.53 + 0.008i, diameter-to-length ratios of 1/2, 1/1.4, 1, 1.4, and 2, and effective size parameters ranging from 0 to 25. These computations parallel our recent study of Light scattering by polydisperse, randomly oriented spheroids and are used to compare scattering properties of the two classes of simple convex particles. Despite the significant difference in shape between the two particle types (entirely smooth surface for spheroids and sharp rectangular edges for cylinders), the comparison shows rather small differences in the integral photometric characteristics (total optical cross sections, single-scattering albedo, and asymmetry parameter of the phase function) and the phase function. The general patterns of the other elements of the scattering matrix for cylinders and aspect-ratio-equivalent spheroids are also qualitatively similar, although noticeable quantitative differences can be found in some particular cases. In general, cylinders demonstrate much less shape dependence of the elements of the scattering matrix than do spheroids. Our computations show that, like spheroids and bispheres, cylinders with surface-equivalent radii smaller than a wavelength can strongly depolarize backscattered light, thus suggesting that backscattering depolarization for nonspherical particles cannot be universally explained by using only geometric-optics considerations. (C) 1996 Optical Society of America [References: 52]
机译:如Mishchenko [Appl。选择。 32,4652(1993)],以严格计算随机取向的有限圆柱体的光散射。首先,我们讨论特定于有限圆柱体的T矩阵计算的数值方面,并给出简单圆柱体模型的基准计算结果。然后,我们报告了对折射率为1.53 + 0.008i,直径与长度比为1 / 2、1 / 1.4、1、1.4和2的多分散,随机取向圆柱体进行大量计算的结果,有效尺寸参数范围为从0到25。这些计算与我们最近对多分散,随机取向的球体的光散射的研究相似,用于比较两类简单凸颗粒的散射特性。尽管两种类型的粒子在形状上存在显着差异(椭球形的表面非常光滑,圆柱体的矩形边缘非常锋利),但对比显示出整体光度特性(总光学截面,单散射反照率和不对称参数)差异很小。相位函数)和相位函数。圆柱体和长宽比等效球体的散射矩阵的其他元素的一般模式在质量上也相似,尽管在某些特定情况下可以发现明显的数量差异。通常,圆柱体显示的散射矩阵元素的形状依赖性要比椭球小得多。我们的计算表明,像球体和双球体一样,具有等效于表面的半径小于波长的圆柱体可以使后向散射光强烈地消偏振,因此表明非球形粒子的后向散射去偏振不能仅通过几何光学考虑来普遍解释。 (C)1996年美国眼镜学会[参考文献:52]

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