Implicit Solvents for the Polarizable Atomic Multipole AMOEBA Force Field.
Implicit Solvents for the Polarizable Atomic Multipole AMOEBA Force Field.
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DOI:
10.1021/acs.jctc.0c01286
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发表时间:
2021-04-13
影响因子:
5.5
通讯作者:
Schnieders MJ
中科院分区:
文献类型:
--
作者:
Corrigan RA;Qi G;Thiel AC;Lynn JR;Walker BD;Casavant TL;Lagardere L;Piquemal JP;Ponder JW;Ren P;Schnieders MJ
Computational protein design, ab initio protein/RNA folding, and protein-ligand screening can be too computationally demanding for explicit treatment of solvent. For these applications, implicit solvent offers a compelling alternative, which we describe here for the polarizable atomic multipole AMOEBA force field based on three treatments of continuum electrostatics: numerical solutions to the nonlinear and linearized versions the Poisson-Boltzmann equation (PBE), the domain-decomposition Conductor-like Screening Model (ddCOSMO) approximation to the PBE, and the analytic generalized Kirkwood (GK) approximation. The continuum electrostatic models are combined with a nonpolar estimator based on novel cavitation and dispersion terms. Electrostatic model parameters are numerically optimized using a least squares style target function based on a library of 103 small molecule solvation free energy differences. Mean signed errors for the APBS, ddCOSMO, and GK models are 0.05, 0.00, and 0.00 kcal/mol, respectively, while the mean unsigned errors are 0.70, 0.63, and 0.58 kcal/mol, respectively. Validation of the electrostatic response of the resulting implicit solvents, which are available in the Tinker (or Tinker-HP), OpenMM, and Force Field X software packages, is based on comparisons to explicit solvent simulations for a series of proteins and nucleic acids. Overall, the emergence of performative implicit solvent models for polarizable force fields will open the door to their use for folding and design applications.
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