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Analysis of the modified point-matching method in the electrostatic problem for axisymmetric particles

机译:轴对称粒子静电问题的改进点匹配方法分析

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An integral modification of the generalized point-matching method (GPMMi) in the electrostatic problem for axisymmetric particles is developed. Scalar potentials that determine electric fields are represented as expansions in terms of eigenfunctions of the Laplace operator in the spherical coordinate system. Unknown expansion coefficients are determined from infinite systems of linear algebraic equations (ISLAEs), which are obtained from the requirement of a minimum of the integrated residual in the boundary conditions on the particle surface. Matrix elements of ISLAEs and expansion coefficients of the "scattered" field at large index values are analyzed analytically and numerically. It is shown analytically that the applicability condition of the GPMMi coincides with that for the extended boundary conditions method (D center dot D'DDe). As model particles, oblate pseudospheroids with semiaxes a = 1 and b aecurrency sign 1 are considered, which are obtained as a result of the inversion of prolate spheroids with the same semiaxes with respect to the coordinate origin. For pseudospheroids, the range of applicability of the considered methods is determined by the condition . Numerical calculations show that, as a rule, the D center dot D'DDe yields considerably more accurate results in this range, with the time consumption being substantially shorter. Beyond the D center dot D'DDe range of applicability, the GPMMi approach can yield reasonable results for the calculation of the polarizability, which should be considered as approximate and which should be verified with other approaches. For oblate nonconvex pseudospheroids (i.e., at ), it is shown that the spheroidal model works well if pseudospheroids are replaced with ordinary "effective" oblate spheroids. Semiaxes a (ef) and b (ef) of the effective spheroids are determined from the requirement of the particle volumes, as well as from the equality of the maximal longitudinal and transverse dimensions of particles or their lengths. As a result, the polarizability of pseudospheroids can be calculated by simple explicit formulas with an error of about 0.5-2%.
机译:开发了对轴对称粒子的静电问题中的广义点匹配方法(GPMMi)的整体修改。确定电场的标量电势表示为球面坐标系中Laplace算子的本征函数的展开。未知的膨胀系数由线性代数方程式(ISLAE)的无限系统确定,这些系统是根据粒子表面边界条件下的最小积分残差的要求而获得的。对ISLAE的矩阵元素和大索引值下“散布”场的扩展系数进行了分析和数值分析。分析表明,GPMMi的适用条件与扩展边界条件方法(D中心点D'DDe)的适用条件一致。作为模型粒子,考虑具有半轴a = 1和b并发符号1的扁伪球体,它们是通过将具有相同半轴的扁球体相对于坐标原点反转而获得的。对于拟球体,所考虑方法的适用范围由条件决定。数值计算表明,通常,D中心点D'DDe在此范围内得出的结果要精确得多,时间消耗要短得多。除了D中心点D'DDe的适用范围外,GPMMi方法还可以得出合理的极化率计算结果,应将其视为近似值,并应使用其他方法进行验证。对于扁圆非凸拟球体(即at),表明如果将伪球体替换为普通的“有效”扁球体,则球体模型会很好地工作。有效球体的半轴a(ef)和b(ef)是根据粒子体积的要求以及粒子的最大纵向和横向尺寸或它们的长度相等而确定的。结果,可以通过简单的显式公式计算伪球体的极化率,其误差约为0.5-2%。

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