Numerical solution of boundary-integral equations for molecular electrostatics

被引:35
|
作者
Bardhan, Jaydeep P. [1 ,2 ]
机构
[1] Argonne Natl Lab, Biosci Div, Argonne, IL 60439 USA
[2] Rush Univ, Dept Physiol & Mol Biophys, Chicago, IL 60612 USA
来源
JOURNAL OF CHEMICAL PHYSICS | 2009年 / 130卷 / 09期
关键词
POISSON-BOLTZMANN EQUATION; POLARIZABLE CONTINUUM MODEL; IMPLICIT SOLVENT MODELS; ELEMENT METHOD; SOLVATION ENERGIES; MACROMOLECULAR ELECTROSTATICS; DIELECTRIC-CONSTANTS; BIOMOLECULAR SYSTEMS; PROTEIN STRUCTURES; AB-INITIO;
D O I
10.1063/1.3080769
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Numerous molecular processes, such as ion permeation through channel proteins, are governed by relatively small changes in energetics. As a result, theoretical investigations of these processes require accurate numerical methods. In the present paper, we evaluate the accuracy of two approaches to simulating boundary-integral equations for continuum models of the electrostatics of solvation. The analysis emphasizes boundary-element method simulations of the integral-equation formulation known as the apparent-surface-charge (ASC) method or polarizable-continuum model (PCM). In many numerical implementations of the ASC/PCM model, one forces the integral equation to be satisfied exactly at a set of discrete points on the boundary. We demonstrate in this paper that this approach to discretization, known as point collocation, is significantly less accurate than an alternative approach known as qualocation. Furthermore, the qualocation method offers this improvement in accuracy without increasing simulation time. Numerical examples demonstrate that electrostatic part of the solvation free energy, when calculated using the collocation and qualocation methods, can differ significantly; for a polypeptide, the answers can differ by as much as 10 kcal/mol (approximately 4% of the total electrostatic contribution to solvation). The applicability of the qualocation discretization to other integral-equation formulations is also discussed, and two equivalences between integral-equation methods are derived. (C) 2009 American Institute of Physics. [DOI:10.1063/1.3080769]
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页数:13
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