Update to the General Amber Force Field for Small Solutes with an Emphasis on Free Energies of Hydration

2014 ◽  
Vol 118 (14) ◽  
pp. 3793-3804 ◽  
Author(s):  
Joakim P. M. Jämbeck ◽  
Alexander P. Lyubartsev
ADMET & DMPK ◽  
2020 ◽  
Author(s):  
Andreas Mecklenfeld ◽  
Gabriele Raabe

<p class="ADMETabstracttext">Rational drug design featuring explicit solubility considerations can greatly benefit from molecular dynamics simulations, as they allow for the prediction of the Gibbs free energy of solvation and thus relative solubilities. In our previous work (A. Mecklenfeld, G. Raabe. J. Chem. Theory Comput. <strong>13 </strong>no. 12 (2017) 6266–6274), we have compared solvation free energy results obtained with the General Amber Force Field (GAFF) and its default restrained electrostatic potential (RESP) partial charges to those obtained by modified implicitly polarized charges (IPolQ-Mod) for an implicit representation of impactful polarization effects. In this work, we have adapted Lennard-Jones parameters for GAFF atom types in combination with IPolQ-Mod to further improve the accuracies of solvation free energy and liquid density predictions. We thereby focus on prominent atom types in common drugs. For the refitting, 357 respectively 384 systems were considered for free energies and densities and validation was performed for 142 free energies and 100 densities of binary mixtures. By the in-depth comparison of simulation results for default GAFF, GAFF with IPolQ-Mod and our new set of parameters, which we label GAFF/IPolQ-Mod+LJ-Fit, we can clearly highlight the improvements of our new model for the description of both relative solubilities and fluid phase behaviour.</p>


2014 ◽  
Vol 10 (8) ◽  
pp. 3570-3577 ◽  
Author(s):  
Silvia A. Martins ◽  
Sergio F. Sousa ◽  
Maria João Ramos ◽  
Pedro A. Fernandes

2021 ◽  
Author(s):  
Andreia Fortuna ◽  
Paulo J. Costa

<div>In force field methods, the usage of off-center point-charges, also called extra-points (EPs), is a common strategy to tackle the anisotropy of the electrostatic potential of covalently-bonded halogens (X), thus allowing the description of halogen bonds (XBs) at the molecular mechanics / molecular dynamics (MM/MD) level. Diverse EP implementations exist in the literature differing on the charge sets and/or the X–EP distances. Poisson–Boltzmann and surface area (PBSA) calculations can be used to obtain solvation free energies (∆G solv ) of small molecules, often to compute binding free energies (∆G bind ) at the MM PBSA level. This method depends, among other parameters, on the empirical assignment of atomic radii (PB radii). Given the multiplicity of off-center point-charges models and the lack of specific PB radii for halogens compatible with such implementations, in this work we assessed the performance of PBSA calculations for the estimation of ∆G solv values in water (∆G hyd ), also conducting an optimization of the halogen PB radii (Cl, Br, and I) for each EP model. We not only expand the usage of EP models in the scope of the General AMBER Force Field (GAFF) but also provide the first optimized halogen PB radii in the context of the CHARMM General Force Field (CGenFF), thus contributing to improving the description of halogenated compounds in PBSA calculations.</div>


2021 ◽  
Author(s):  
Andreia Fortuna ◽  
Paulo J. Costa

<div>In force field methods, the usage of off-center point-charges, also called extra-points (EPs), is a common strategy to tackle the anisotropy of the electrostatic potential of covalently-bonded halogens (X), thus allowing the description of halogen bonds (XBs) at the molecular mechanics / molecular dynamics (MM/MD) level. Diverse EP implementations exist in the literature differing on the charge sets and/or the X–EP distances. Poisson–Boltzmann and surface area (PBSA) calculations can be used to obtain solvation free energies (∆G solv ) of small molecules, often to compute binding free energies (∆G bind ) at the MM PBSA level. This method depends, among other parameters, on the empirical assignment of atomic radii (PB radii). Given the multiplicity of off-center point-charges models and the lack of specific PB radii for halogens compatible with such implementations, in this work we assessed the performance of PBSA calculations for the estimation of ∆G solv values in water (∆G hyd ), also conducting an optimization of the halogen PB radii (Cl, Br, and I) for each EP model. We not only expand the usage of EP models in the scope of the General AMBER Force Field (GAFF) but also provide the first optimized halogen PB radii in the context of the CHARMM General Force Field (CGenFF), thus contributing to improving the description of halogenated compounds in PBSA calculations.</div>


2021 ◽  
Author(s):  
Andreia Fortuna ◽  
Paulo J. Costa

<div>In force field methods, the usage of off-center point-charges, also called extra-points (EPs), is a common strategy to tackle the anisotropy of the electrostatic potential of covalently-bonded halogens (X), thus allowing the description of halogen bonds (XBs) at the molecular mechanics / molecular dynamics (MM/MD) level. Diverse EP implementations exist in the literature differing on the charge sets and/or the X–EP distances. Poisson–Boltzmann and surface area (PBSA) calculations can be used to obtain solvation free energies (∆G solv ) of small molecules, often to compute binding free energies (∆G bind ) at the MM PBSA level. This method depends, among other parameters, on the empirical assignment of atomic radii (PB radii). Given the multiplicity of off-center point-charges models and the lack of specific PB radii for halogens compatible with such implementations, in this work we assessed the performance of PBSA calculations for the estimation of ∆G solv values in water (∆G hyd ), also conducting an optimization of the halogen PB radii (Cl, Br, and I) for each EP model. We not only expand the usage of EP models in the scope of the General AMBER Force Field (GAFF) but also provide the first optimized halogen PB radii in the context of the CHARMM General Force Field (CGenFF), thus contributing to improving the description of halogenated compounds in PBSA calculations.</div>


2018 ◽  
Author(s):  
Maximiliano Riquelme ◽  
Alejandro Lara ◽  
David L. Mobley ◽  
Toon Vestraelen ◽  
Adelio R Matamala ◽  
...  

<div>Computer simulations of bio-molecular systems often use force fields, which are combinations of simple empirical atom-based functions to describe the molecular interactions. Even though polarizable force fields give a more detailed description of intermolecular interactions, nonpolarizable force fields, developed several decades ago, are often still preferred because of their reduced computation cost. Electrostatic interactions play a major role in bio-molecular systems and are therein described by atomic point charges.</div><div>In this work, we address the performance of different atomic charges to reproduce experimental hydration free energies in the FreeSolv database in combination with the GAFF force field. Atomic charges were calculated by two atoms-in-molecules approaches, Hirshfeld-I and Minimal Basis Iterative Stockholder (MBIS). To account for polarization effects, the charges were derived from the solute's electron density computed with an implicit solvent model and the energy required to polarize the solute was added to the free energy cycle. The calculated hydration free energies were analyzed with an error model, revealing systematic errors associated with specific functional groups or chemical elements. The best agreement with the experimental data is observed for the MBIS atomic charge method, including the solvent polarization, with a root mean square error of 2.0 kcal mol<sup>-1</sup> for the 613 organic molecules studied. The largest deviation was observed for phosphor-containing molecules and the molecules with amide, ester and amine functional groups.</div>


2012 ◽  
Vol 8 (3) ◽  
pp. 948-958 ◽  
Author(s):  
Arnau Cordomí ◽  
Gianluigi Caltabiano ◽  
Leonardo Pardo

2004 ◽  
Vol 108 (41) ◽  
pp. 16264-16270 ◽  
Author(s):  
William L. Jorgensen ◽  
Jakob P. Ulmschneider ◽  
Julian Tirado-Rives

2016 ◽  
Vol 56 (4) ◽  
pp. 811-818 ◽  
Author(s):  
Suqing Zheng ◽  
Qing Tang ◽  
Jian He ◽  
Shiyu Du ◽  
Shaofang Xu ◽  
...  

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