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The Numerical Solution of the Nonlinear Poisson-Boltzmann Equation Under the Anisotropic Boundary Condition for Colloidal Plasmas

机译:各向异性边界条件下胶体等离子体非线性泊松-玻尔兹曼方程的数值解

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摘要

Based on the model of the Wigner-Seitz cell, the surface potential of the spherical macroparticle (radius a) expands in terms of the monopole (q). A dipole (p) model is assumed for ananisotropic boundary condition of the nonlinear Poisson-Boltzmann equation. Using the finite element method implemented by the FlexPDE software, the potential distribution around the macroparticle is obtained for different ratios p/qa. The calculated results for the potential show that there is attractive region in the vicinity of the macroparticle when vertical bar p/qa vertical bar>1.1, and noticeably there is a potential well behind the macroparticle when vertical bar p/qa vertical bar=1.1, i.e., there exists both an attractive region and a repulsive region simultaneously. This means that the attractive interaction between macroparticles may arise from the anisotropic distribution of the surrounding plasmas, which well explains some experimental observations.
机译:基于Wigner-Seitz细胞模型,球形大颗粒(半径a)的表面电势以单极(q)的形式扩展。对于非线性Poisson-Boltzmann方程的各向异性边界条件,假设有一个偶极(p)模型。使用由FlexPDE软件实现的有限元方法,可以获得p / qa不同比率的大颗粒周围的电势分布。势的计算结果表明,当垂直线p / qa垂直线> 1.1时,在大颗粒附近有一个吸引区域,而当垂直线p / qa垂直线= 1.1时,在大颗粒的后面有一个明显的电位,即,同时存在吸引区域和排斥区域。这意味着大颗粒之间的吸引力相互作用可能来自周围等离子体的各向异性分布,这很好地解释了一些实验观察结果。

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