Molecular dynamics simulations of peptides and proteins with a continuum electrostatic model based on screened Coulomb potentials
Authors: Hassan Sergio A. , Mehler Ernest L. , Zhang Daqun , Weinstein Harel 
Published: February 2003

AbstractA continuum electrostatics approach for molecular dynamics (MD) simulations of macromolecules is presented and analyzed for its performance on a peptide and a globular protein. The approach incorporates the screened Coulomb potential (SCP) continuum model of electrostatics, which was reported earlier. The model was validated in a broad set of tests some of which were based on Monte Carlo simulations that included single amino acids, peptides, and proteins. The implementation for large‐scale MD simulations presented in this article is based on a pairwise potential that makes the electrostatic model suitable for fast analytical calculation of forces. To assess the suitability of the approach, a preliminary validation is conducted, which consists of (i) a 3‐ns MD simulation of the immunoglobulin‐binding domain of streptococcal protein G, a 56‐residue globular protein and (ii) a 3‐ns simulation of Dynorphin, a biological peptide of 17 amino acids. In both cases, the results are compared with those obtained from MD simulations using explicit water (EW) molecules in an all‐atom representation. The initial structure of Dynorphin was assumed to be an α‐helix between residues 1 and 9 as suggested from NMR measurements in micelles. The results obtained in the MD simulations show that the helical structure collapses early in the simulation, a behavior observed in the EW simulation and consistent with spectroscopic data that suggest that the peptide may adopt mainly an extended conformation in water. The dynamics of protein G calculated with the SCP implicit solvent model (SCP‐ISM) reveals a stable structure that conserves all the elements of secondary structure throughout the entire simulation time. The average structures calculated from the trajectories with the implicit and explicit solvent models had a cRMSD of 1.1 Å, whereas each average structure had a cRMSD of about 0.8Å with respect to the X‐ray structure. The main conformational differences of the average structures with respect to the crystal structure occur in the loop involving residues 8–14. Despite the overall similarity of the simulated dynamics with EW and SCP models, fluctuations of side‐chains are larger when the implicit solvent is used, especially in solvent exposed side‐chains. The MD simulation of Dynorphin was extended to 40 ns to study its behavior in an aqueous environment. This long simulation showed that the peptide has a tendency to form an α‐helical structure in water, but the stabilization free energy is too weak, resulting in frequent interconversions between random and helical conformations during the simulation time. The results reported here suggest that the SCP implicit solvent model is adequate to describe electrostatic effects in MD simulation of both peptides and proteins using the same set of parameters. It is suggested that the present approach could form the basis for the development of a reliable and general continuum approach for use in molecular biology, and directions are outlined for attaining this long‐term goal. Proteins 2003;51:109–125. © 2003 Wiley‐Liss, Inc.