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一种用于计算任意表面拓扑结构胶体颗粒间静电相互作用的模型。

A Model for Calculating Electrostatic Interactions between Colloidal Particles of Arbitrary Surface Topology.

作者信息

Sun Ning, Walz John Y.

机构信息

Department of Chemical Engineering, Yale University, New Haven, Connecticut, 06520

出版信息

J Colloid Interface Sci. 2001 Feb 1;234(1):90-105. doi: 10.1006/jcis.2000.7248.

Abstract

A numerical model for calculating the electrostatic interaction between two particles of arbitrary shape and topology is described. A key feature of the model is a generalized discretization program, capable of simulating any desired analytical shape as a set of flat, triangular elements. The relative sizes of the elements are adjusted using a density function to better match the desired shape and the spatial variation of the electrical surface properties on each particle. The distribution of either surface potential or surface charge density is then calculated using a boundary element approach to solve the linearized Poisson-Boltzmann equation. Example interaction energy profiles are calculated for three different types of roughness-bumps, pits, and surface waves. It is found that the interaction energy between rough particles remains different from that between two equivalent smooth spheres at all separations, even for gap widths much larger than either the solution Debye length or the characteristic roughness size. This behavior at large gap widths arises from the nature of the decay of the electric potential away from each particle. In addition, the magnitude of the roughness effect is found to depend greatly on the size and shape of the nonuniformity as well as the electrostatic boundary conditions. For example, for a sphere containing asperities of height equal to 0.2 times the particle radius, the interaction energy can be as much as 50% greater than that between two equivalent spheres under the condition of constant surface potential. At constant surface charge density, the ratio of the interaction energies between rough and smooth spheres was found to either diverge or become zero as contact between the two particles is approached, depending on the nature of the roughness. Changes of this magnitude could clearly have a substantial impact on the stability behavior of a dispersion of such particles. Copyright 2001 Academic Press.

摘要

本文描述了一种用于计算任意形状和拓扑结构的两个粒子之间静电相互作用的数值模型。该模型的一个关键特性是一个广义离散化程序,它能够将任何所需的解析形状模拟为一组扁平的三角形单元。使用密度函数调整单元的相对大小,以更好地匹配所需形状以及每个粒子上电表面性质的空间变化。然后,使用边界元方法求解线性化的泊松 - 玻尔兹曼方程,计算表面电势或表面电荷密度的分布。针对三种不同类型的粗糙度——凸起、凹坑和表面波,计算了相互作用能分布示例。研究发现,即使间隙宽度远大于溶液德拜长度或特征粗糙度尺寸,粗糙粒子之间的相互作用能在所有间距下都与两个等效光滑球体之间的相互作用能不同。这种在大间隙宽度下的行为源于电势从每个粒子处衰减的性质。此外,发现粗糙度效应的大小在很大程度上取决于不均匀性的大小和形状以及静电边界条件。例如,对于一个包含高度等于粒子半径0.2倍的粗糙物的球体,在恒定表面电势条件下,其相互作用能可能比两个等效球体之间的相互作用能大50%。在恒定表面电荷密度下,粗糙球体与光滑球体之间相互作用能的比值在接近两个粒子接触时,根据粗糙度的性质,要么发散要么变为零。这种量级的变化显然会对这种粒子分散体的稳定性行为产生重大影响。版权所有2001年学术出版社。

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