4.7 Article

Polarizable Force Field for Peptides and Proteins Based on the Classical Drude Oscillator

Journal

JOURNAL OF CHEMICAL THEORY AND COMPUTATION
Volume 9, Issue 12, Pages 5430-5449

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/ct400781b

Keywords

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Funding

  1. NIH [GM072558]
  2. National Science Foundation [OCI-1053575]
  3. Swiss National Science Foundation Fellowship [PBBSP2_144301]
  4. Office of Science of the U.S. Department of Energy [DE-AC02-06CH11357]
  5. University of Maryland Computer-Aided Drug Design Center and the Extreme Science and Engineering Discovery Environment (XSEDE)
  6. Argonne Leadership Computing Facility (ALCF) at Argonne National Laboratory
  7. Swiss National Science Foundation (SNF) [PBBSP2_144301] Funding Source: Swiss National Science Foundation (SNF)

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Presented is a polarizable force field based on a classical Drude oscillator framework, currently implemented in the programs CHARMM and NAMD, for modeling and molecular dynamics (MD) simulation studies of peptides and proteins. Building upon parameters for model compounds representative of the functional groups in proteins, the development of the force field focused on the optimization of the parameters for the polypeptide backbone and the connectivity between the backbone and side chains. Optimization of the backbone electrostatic parameters targeted quantum mechanical conformational energies, interactions with water, molecular dipole moments and polarizabilities, and experimental condensed phase data for short polypeptides such as (Ala)(5). Additional optimization of the backbone phi, psi conformational preferences included adjustments of the tabulated two-dimensional spline function through the CMAP term. Validation of the model included simulations of a collection of peptides and proteins. This first generation polarizable model is shown to maintain the folded state of the studied systems on the 100 ns time scale in explicit solvent MD simulations. The Drude model typically yields larger RMS differences as compared to the additive CHARMM36 force field (C36) and shows additional flexibility as compared to the additive model. Comparison with NMR chemical shift data shows a small degradation of the polarizable model with respect to the additive, though the level of agreement may be considered satisfactory. However, the polarizable model shows improvement for the residues with significantly underestimated S-2 order parameters in the additive model. Analysis of dipole moments associated with the peptide backbone and tryptophan side chains show the Drude model to have considerably larger values than those present in C36, with the dipole moments of the peptide backbone enhanced to a greater extent in sheets versus helices and the dipoles of individual moieties observed to undergo large variations during the MD simulations. Although there are still some limitations, the presented model, termed Drude-2013, is anticipated to yield a molecular picture of peptide and protein structure and function that will be of increased physical validity and internal consistency in a computationally accessible fashion.

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