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首页> 外文期刊>Journal of Quantitative Spectroscopy & Radiative Transfer >Energy density density distribution of light inside two-dimensional randomly scattering slabs illuminated by a plane wave
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Energy density density distribution of light inside two-dimensional randomly scattering slabs illuminated by a plane wave

机译:平面波照射二维随机散射板内的光的能量密度密度分布

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In this study, light scattering inside random two-dimensional media, illuminated by an incident plane wave, is simulated by numerically solving Maxwell's equations. The results are compared to the corresponding, newly derived analytical solution of the radiative transfer equation (RTE) for a laterally infinitely extended slab. The two-dimensional scattering medium consists of a random distribution of circular scatterers with well-defined optical properties and area fraction. The ensemble-averaged energy density calculated from the electromagnetic fields obtained from Maxwell's equations is compared with the energy density obtained from the two-dimensional radiative transfer equation. Simulations for different area fractions show good agreement of the energy densities of the two theories for small area fractions (< 0.2) of the scatterers. For low concentrations, three different slab thicknesses are examined. The ensemble-averaged energy density calculated with Maxwell's equations show good agreement for all three slab thicknesses compared with the energy density obtained with the RTE. The results of this study can be used to calculate the average energy density distribution of light inside slabs of fiber-like structures with fast calculations of the presented analytical RTE solution. (C) 2019 Elsevier Ltd. All rights reserved.
机译:在该研究中,通过数值求解麦克斯韦方程来模拟由入射平面波照亮的随机二维介质内的光散射。将结果与横向无限延伸的板坯的辐射转移方程(RTE)的相应的新推导的分析解进行比较。二维散射介质由具有明确定义的光学性质和面积分数的圆形散射仪的随机分布组成。将由麦克斯韦方程获得的电磁场计算的集合平均能量密度与从二维辐射传输方程获得的能量密度进行比较。不同面积分数的模拟显示了散射体的小面积分数(<0.2)的两个理论的能量密度吻合良好。对于低浓度,检查三种不同的板坯厚度。与Maxwell等式计算的集合平均能量密度显示所有三个板坯厚度的良好一致性,与RTE获得的能量密度相比。该研究的结果可用于计算纤维状结构的光线内部的平均能量密度分布,并快速计算所呈现的分析RTE溶液。 (c)2019年elestvier有限公司保留所有权利。

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