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优先溶剂化的高级介电连续介质模型。

Advanced dielectric continuum model of preferential solvation.

作者信息

Basilevsky Mikhail, Odinokov Alexey, Nikitina Ekaterina, Grigoriev Fedor, Petrov Nikolai, Alfimov Mikhail

机构信息

Photochemistry Center, Russian Academy of Sciences, Moscow 119421, Russia.

出版信息

J Chem Phys. 2009 Jan 14;130(2):024505. doi: 10.1063/1.3010706.

Abstract

A continuum model for solvation effects in binary solvent mixtures is formulated in terms of the density functional theory. The presence of two variables, namely, the dimensionless solvent composition y and the dimensionless total solvent density z, is an essential feature of binary systems. Their coupling, hidden in the structure of the local dielectric permittivity function, is postulated at the phenomenological level. Local equilibrium conditions are derived by a variation in the free energy functional expressed in terms of the composition and density variables. They appear as a pair of coupled equations defining y and z as spatial distributions. We consider the simplest spherically symmetric case of the Born-type ion immersed in the benzene/dimethylsulfoxide (DMSO) solvent mixture. The profiles of y(R) and z(R) along the radius R, which measures the distance from the ion center, are found in molecular dynamics (MD) simulations. It is shown that for a given solute ion z(R) does not depend significantly on the composition variable y. A simplified solution is then obtained by inserting z(R), found in the MD simulation for the pure DMSO, in the single equation which defines y(R). In this way composition dependences of the main solvation effects are investigated. The local density augmentation appears as a peak of z(R) at the ion boundary. It is responsible for the fine solvation effects missing when the ordinary solvation theories, in which z=1, are applied. These phenomena, studied for negative ions, reproduce consistently the simulation results. For positive ions the simulation shows that z>>1 (z=5-6 at the maximum of the z peak), which means that an extremely dense solvation shell is formed. In such a situation the continuum description fails to be valid within a consistent parametrization.

摘要

基于密度泛函理论建立了二元溶剂混合物中溶剂化效应的连续介质模型。二元体系的一个基本特征是存在两个变量,即无量纲溶剂组成y和无量纲总溶剂密度z。它们的耦合隐藏在局部介电常数函数的结构中,在唯象层面上进行了假设。通过以组成和密度变量表示的自由能泛函的变分导出局部平衡条件。它们表现为一对耦合方程,将y和z定义为空间分布。我们考虑了浸没在苯/二甲基亚砜(DMSO)溶剂混合物中的Born型离子的最简单球对称情况。在分子动力学(MD)模拟中发现了沿半径R(测量到离子中心的距离)的y(R)和z(R)的分布。结果表明,对于给定的溶质离子,z(R)对组成变量y的依赖性不显著。然后,通过将MD模拟中纯DMSO的z(R)代入定义y(R)的单个方程中,得到了一个简化解。通过这种方式研究了主要溶剂化效应的组成依赖性。局部密度增加表现为离子边界处z(R)的一个峰值。它导致了应用普通溶剂化理论(其中z = 1)时所缺失的精细溶剂化效应。对负离子研究的这些现象与模拟结果一致。对于正离子,模拟表明z >> 1(z峰值最大时z = 5 - 6),这意味着形成了一个极其致密的溶剂化壳层。在这种情况下,连续介质描述在一致的参数化范围内失效。

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