Literature DB >> 4046024

On the calculation of electrostatic interactions in proteins.

M K Gilson, A Rashin, R Fine, B Honig.   

Abstract

In this paper we present a classical treatment of electrostatic interactions in proteins. The protein is treated as a region of low dielectric constant with spherical charges embedded within it, surrounded by an aqueous solvent of high dielectric constant, which may contain a simple electrolyte. The complete analysis includes the effects of solvent screening, polarization forces, and self energies, which are related to solvation energies. Formulae, and sample calculations of forces and energies, are given for the special case of a spherical protein. Our analysis and model calculations point out that any consistent treatment of electrostatic interactions in proteins should account for the following. Solvent polarization is an important factor in the calculation of pairwise electrostatic interactions. Solvent polarization substantially affects both electrostatic energies and forces acting upon charges. No simple expression for the effective dielectric constant, Deff, can generally be valid, since Deff is a sensitive function of position. Solvent screening of pairwise interactions involving dipolar groups is less effective than the screening of charges. In fact for many interactions involving dipoles, solvent screening can be essentially ignored. The self energy of charges makes a large contribution to the total electrostatic energy of a protein. This must be compensated by specific interactions with other groups in the protein. Strategies for applying our analysis to proteins whose structures are known are discussed.

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Year:  1985        PMID: 4046024     DOI: 10.1016/0022-2836(85)90297-9

Source DB:  PubMed          Journal:  J Mol Biol        ISSN: 0022-2836            Impact factor:   5.469


  57 in total

1.  Tanford-Kirkwood electrostatics for protein modeling.

Authors:  J J Havranek; P B Harbury
Journal:  Proc Natl Acad Sci U S A       Date:  1999-09-28       Impact factor: 11.205

2.  Thermodynamic linkage between the binding of protons and inhibitors to HIV-1 protease.

Authors:  J Trylska; J Antosiewicz; M Geller; C N Hodge; R M Klabe; M S Head; M K Gilson
Journal:  Protein Sci       Date:  1999-01       Impact factor: 6.725

3.  The role of small intraprotein cavities in the catalytic cycle of bacteriorhodopsin.

Authors:  Ran Friedman; Esther Nachliel; Menachem Gutman
Journal:  Biophys J       Date:  2003-08       Impact factor: 4.033

4.  Influence of the solvent structure on the electrostatic interactions in proteins.

Authors:  Alexander Rubinstein; Simon Sherman
Journal:  Biophys J       Date:  2004-09       Impact factor: 4.033

5.  Chemical space sampling by different scoring functions and crystal structures.

Authors:  Natasja Brooijmans; Christine Humblet
Journal:  J Comput Aided Mol Des       Date:  2010-04-18       Impact factor: 3.686

6.  SAMPL2 and continuum modeling.

Authors:  Anthony Nicholls; Stanislaw Wlodek; J Andrew Grant
Journal:  J Comput Aided Mol Des       Date:  2010-04-06       Impact factor: 3.686

7.  DelPhi Web Server: A comprehensive online suite for electrostatic calculations of biological macromolecules and their complexes.

Authors:  Subhra Sarkar; Shawn Witham; Jie Zhang; Maxim Zhenirovskyy; Walter Rocchia; Emil Alexov
Journal:  Commun Comput Phys       Date:  2013-01       Impact factor: 3.246

8.  Structural determinants of trypsin affinity and specificity for cationic inhibitors.

Authors:  F Polticelli; P Ascenzi; M Bolognesi; B Honig
Journal:  Protein Sci       Date:  1999-12       Impact factor: 6.725

9.  Calculation of absolute protein-ligand binding affinity using path and endpoint approaches.

Authors:  Michael S Lee; Mark A Olson
Journal:  Biophys J       Date:  2005-11-11       Impact factor: 4.033

10.  Solvation free energies of alanine peptides: the effect of flexibility.

Authors:  Hironori Kokubo; Robert C Harris; Dilipkumar Asthagiri; B Montgomery Pettitt
Journal:  J Phys Chem B       Date:  2013-12-13       Impact factor: 2.991

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