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通过实验测出532 nm激光在近地大气的角散射系数,对Junge和Deirmendjian两种模型的气溶胶系统在不同的系统参数、不同的折射率的情况下的散射相函数进行了计算,发现与实验所测得的曲线有明显的差异,这两种模型都不存在散射次极峰.通过对不同半径粒子的散射相函数的计算,说明实验所测的气溶胶系统在粒子尺寸较大的区间的密度要比Junge和Deirmendjian两种模型的密度要大得多,在假定大粒子服从正态分布的前提下,拟合出了气溶胶的分布函数.

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