Construction of Multi-Scale Dissipative Particle Dynamics (DPD) Models from other Coarse-Grained Models

24 January 2024, Version 1
This content is a preprint and has not undergone peer review at the time of posting.

Abstract

We present a general scheme for converting coarse grained models into Dissipative Particle Dynamics (DPD) models. We build the corresponding DPD models by anal- ogy with the de novo DPD coarse graining scheme suggested by Groot and Warren (J. Chem. Phys., 1997). Electrostatic interactions between charged DPD particles are represented though the addition of a long-range Slater Coulomb potential as suggested by Gonz ́alez-Melchor et al (J. Chem. Phys 2006). The construction is illustrated by converting MARTINI models for various proteins into a DPD representation, but it not restricted to the usual potential form in the MARTINI model—viz Lennard-Jones potentials. We further extended the DPD scheme away from the typical use of homo- geneous particle sizes, and therefor faithfully representing the variations in the particle sizes seen in the underlying MARTINI model. The accuracy of the resulting construc- tion of our generalized DPD models with respect to several structural observables have been benchmarked favorably against all-atom and MARTINI models for a selected set of peptides and proteins, and variations in the scales of the coarse-graining of the water solvent.

Keywords

Dissipative Particle Dynamics
coarse-graining
protein structure
MARTINI force fields

Supplementary materials

Title
Description
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Title
Supporting Information for “A Generalized Representation of Multi-scale Coarse Grained Molecular Model Using Dissipative Particle Dynamics (DPD)”
Description
The parameters for the Dissipative Particle Dynamics (DPD) models reported in the main paper are included in Sec. 2. In addition, comparisons for the radius of gyration verses RMSD and RSMF verses residue across the various representations—all-atom, MARTINI, DPD(ρwater = 3), and DPD(ρwater = 20)—for each of the proteins explored in this work are included in Sec. 3.
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