Revised 4-point Water Model for the Classical Drude Oscillator Polarizable Force Field: SWM4-HLJ

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

Abstract

In this work the 4-point polarizable SWM4 Drude water model is reparametrized. Multiple models were developed using different strategies towards reproduction of specific target data. Results indicate that no individual model can reproduce all the selected target data in the context of the present form of the potential energy function. The changes considered in the new models include, 1) variations in the gas phase dipole moment, 2) variations in the molecular polarizability, 3) variations of the distance between the oxygen and the M site, 4) variation of the oxygen Lennard-Jones (LJ) parameters, 5) introduction of a LJ potential to the hydrogen atoms, and 6) variations of the H-O-H angle. Detailed analysis is presented for 3 new water models from which a final model, SWM4-HLJ, is selected as the future default model for the Drude polarizable force field. The model maintains the gas phase dipole moment as the experimental value while the remaining listed terms were adjusted including a larger H-O-H angle (108.12°). Compared to its predecessor, SWM4-NDP, the self-diffusion coefficient, water dimer properties, and water cluster energies are greatly improved. The temperature dependence of the density of the new model also performs better. Overall, the new SWM4-HLJ water model is a general improvement and a good balance between microscopic and bulk properties is achieved.

Supplementary materials

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Supporting information
Description
The supporting information contains equations S1 and S2 for calculation of the isothermal compressibility and heat capacity, respectively, Table S1 includes the gas phase and condensed phase dipole moments of the water models, Figures S1, S2, and S3 are bulk properties of the SWM4-NDP model as a function of temperature compared to those of the ML1, ML2 and SWM4-HLJ water models, respectively, Figure S4 is the heat capacity of the water models, Figure S5 is the dipole moment distributions of the water models from bulk simulations, and Figure S6 shows convergence of the viscosity of SWM4-HLJ water model.
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