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理论描述任意大小和电荷非对称的 n 种离子混合物的双电层。I. 球形几何。

Theoretical description of the electrical double layer for a mixture of n ionic species with arbitrary size and charge asymmetries. I. Spherical geometry.

机构信息

Instituto de Física de la Universidad Autónoma de San Luis Potosí, Álvaro Obregón 64, 78000 San Luis Potosí, Mexico.

Facultad de Ciencias de la Universidad Autónoma de San Luis Potosí, Av. Chapultepec 1570, Privadas del Pedregal, 78295 San Luis Potosí, Mexico.

出版信息

J Chem Phys. 2023 Jun 14;158(22). doi: 10.1063/5.0151140.

Abstract

In this work, we propose a theoretical finite element description of the ionic profiles of a general mixture of n species of spherical charged particles dissolved in an implicit solvent, with arbitrary size and charge asymmetries, neutralizing a spherical macroion. This approach aims to close the gap between the nano- and the micro-scales in macroion solutions, taking into account the ion correlations and ionic excluded volume effects consistently. When these last two features are neglected, the classical non-linear Poisson-Boltzmann theory for n ionic species-with different ionic closest approach distances to the colloidal surface-is recovered as a limit case. As a proof of concept, we study the electrical double layer of an electroneutral mixture of oppositely charged colloids and small microions, with an asymmetry 1:333 in size and 1:10 in valence, in salt-free and added salt environments. Our theoretical approach displays a good agreement regarding the ionic profiles, the integrated charge, and the mean electrostatic potential obtained from molecular dynamics simulations with explicit-sized microions. Although the non-linear Poisson-Boltzmann colloid-colloid and colloid-microion profiles differ notably from those obtained via molecular dynamics simulations with explicit small-sized ions, the associated mean electrostatic potential agrees well with the corresponding explicit microion simulations.

摘要

在这项工作中,我们提出了一种理论有限元描述,用于描述溶解在隐溶剂中的 n 种球形带电粒子的一般混合物的离子分布,其中包括任意大小和电荷不对称性,中和一个球形大分子。这种方法旨在弥合纳米和微观尺度之间的差距,一致考虑离子相关性和离子排斥体积效应。当忽略后两个特征时,对于 n 种具有不同离子最近距离到胶体表面的离子,经典的非线性泊松-玻尔兹曼理论是一个极限情况。作为概念验证,我们研究了带相反电荷的胶体和小微离子的电双层,其大小和价数的不对称性分别为 1:333 和 1:10,在无盐和加盐环境下。我们的理论方法在离子分布、积分电荷和从具有显式尺寸微离子的分子动力学模拟中获得的平均静电势方面显示出良好的一致性。尽管非线性泊松-玻尔兹曼胶体-胶体和胶体-微离子分布与通过具有显式小尺寸离子的分子动力学模拟得到的分布有显著差异,但相关的平均静电势与对应的显式微离子模拟吻合良好。

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