首页> 外文期刊>Journal of the Optical Society of America, A. Optics, image science, and vision >Extinction of light in dispersive media with high particle concentrations: applicability limits of the interference approximation
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Extinction of light in dispersive media with high particle concentrations: applicability limits of the interference approximation

机译:高粒子浓度分散介质中的光消光:干涉近似的适用范围

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We investigated the limits of applicability of the interference approximation (ITA), which is orten used to calculate light fields in dispersive media with high particle concentrations. We analyzed the conditions under which the use of the ITA leads to an error in calculation of the dispersive-medium extinction coefficient ∈ equal to 10%, 15%, and 25%. The analysis was carried out by comparing the values of ∈ calculated in the ITA with the results of the calculation of ∈ in a much more exact quasi-crystalline approximation (QCA). The validity of the QCA in estimating the error of the ITA is shown by comparing the values of ∈ calculated in the ITA and the QCA with experimental data [J. Opt. Soc. Am. 72, 1317 (1982)]. Our investigation shows that the ITA can be used only at relatively small values of the particle size parameter x. When the relative refractive index of the particles is n approx.> 1.8, the applicability of the ITA is limited to the case in which the particle size parameter x ≤ x_(max) ≈ 1.5. A decrease in n leads to an increase in x_(max), and for nonabsorbing particles at n approx.<1.3, x_(max) is approximately proportional: 1/(n - 1). An increase in the imaginary part of the relative refractive index of the particles k leads to a decrease in x_(max). The smaller the n, the greater the dependence of x_(max) on k.
机译:我们研究了干扰近似法(ITA)的适用范围,该方法通常用于计算具有高粒子浓度的分散介质中的光场。我们分析了使用ITA导致计算分散介质消光系数ε等于10%,15%和25%的误差的条件。通过以更精确的准晶体近似(QCA)比较ITA中计算的ε值与ε的计算结果来进行分析。通过比较ITA和QCA中计算出的ε值与实验数据,可以证明QCA在估计ITA误差中的有效性[J.选择。 Soc。上午。 72,1317(1982)]。我们的研究表明,ITA只能在相对较小的粒度参数x值下使用。当颗粒的相对折射率为n约> 1.8时,ITA的适用性限于粒径参数x≤x_(max)≈1.5的情况。 n的减少导致x_(max)的增加,对于n小于<1.3的非吸收颗粒,x_(max)近似成比例:1 /(n-1)。粒子k的相对折射率的虚部的增加导致x_(max)的减小。 n越小,x_(max)对k的依赖性越大。

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