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LIGHT SCATTERING BY A CORE-MANTLE SPHEROIDAL PARTICLE

机译:地幔球状粒子的光散射

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A solution of the electromagnetic scattering problem for confocal coated spheroids has been obtained by the method of separation of variables in a spheroidal coordinate system. The main features of the solution are (i) the incident, scattered, and internal radiation fields are divided into two parts: an axisymmetric part independent of the azimuthal angle phi and a nonaxisymmetric part that with integration over ip gives zero; the diffraction problems for each part are solved separately; (ii) the scalar potentials of the solution are chosen in a special way: Abraham's potentials (for the axisymmetric part) and a superposition of the potentials used for spheres and infinitely long cylinders (for the nonaxisymmetric part). Such a procedure has been applied to homogeneous spheroids [Differential Equations 19, 1765 (1983); Astrophys. Space Sci. 204, 19, (1993)] and allows us to solve the light scattering problem for confocal spheroids with an arbitrary refractive index, size, and shape of the core or mantle. Numerical tests are described in detail. The efficiency factors have been calculated for prolate and oblate spheroids with refractive indices of 1.5 +/- 0.0i, 1.5 + 0.05i for the core and refractive indices of 1.3 + 0.0i, 1.3 + 0.05i for the mantle. The effects of the core size and particle shape as well as those of absorption in the core or mantle are examined. It is found that the efficiency factors of the coated and homogeneous spheroids with the volume-averaged refractive index are similar to first maximum. [References: 32]
机译:通过在球坐标系中分离变量的方法,已经获得了共焦涂覆球体的电磁散射问题的解决方案。该解决方案的主要特征是:(i)将入射,散射和内部辐射场分为两部分:独立于方位角phi的轴对称部分和在ip上积分为零的非轴对称部分;每个部分的衍射问题分别得到解决。 (ii)以特殊方式选择解的标量势:亚伯拉罕势(对于轴对称部分)以及球体和无限长圆柱体(对于非轴对称部分)使用的势的叠加。这样的程序已经应用于均质球体[Differential Equations 19,1765(1983);天体。太空科学204,19,(1993)],并允许我们解决具有任意折射率,大小或形状的共焦球体的光散射问题。详细描述了数值测试。计算出扁长球和扁长球体的效率因子,纤芯的折射率为1.5 +/- 0.0i,1.5 + 0.05i,地幔的折射率为1.3 + 0.0i,1.3 + 0.05i。检查了核尺寸和颗粒形状以及在核或地幔中吸收的影响。发现具有体积平均折射率的涂覆的和均质的球体的效率因子类似于第一最大值。 [参考:32]

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