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Extension of the TraPPE Force Field for Battery Electrolyte Solvents
[Image: see text] Optimizing electrolyte formulations is key to improving performance of Li-/Na-ion batteries, where transport properties (diffusion coefficient, viscosity) and permittivity need to be predicted as functions of temperature, salt concentration and solvent composition. More efficient a...
Autores principales: | , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2023
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10026065/ https://www.ncbi.nlm.nih.gov/pubmed/36862420 http://dx.doi.org/10.1021/acs.jpcb.2c06993 |
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author | Luo, Zhifen Burrows, Stephen A. Smoukov, Stoyan K. Fan, Xiaoli Boek, Edo S. |
author_facet | Luo, Zhifen Burrows, Stephen A. Smoukov, Stoyan K. Fan, Xiaoli Boek, Edo S. |
author_sort | Luo, Zhifen |
collection | PubMed |
description | [Image: see text] Optimizing electrolyte formulations is key to improving performance of Li-/Na-ion batteries, where transport properties (diffusion coefficient, viscosity) and permittivity need to be predicted as functions of temperature, salt concentration and solvent composition. More efficient and reliable simulation models are urgently needed, owing to the high cost of experimental methods and the lack of united-atom molecular dynamics force fields validated for electrolyte solvents. Here the computationally efficient TraPPE united-atom force field is extended to be compatible with carbonate solvents, optimizing the charges and dihedral potential. Computing the properties of electrolyte solvents, ethylene carbonate (EC), propylene carbonate (PC), dimethyl carbonate (DMC), diethyl carbonate (DEC), and dimethoxyethane (DME), we observe that the average absolute errors in the density, self-diffusion coefficient, permittivity, viscosity, and surface tension are approximately 15% of the corresponding experimental values. Results compare favorably to all-atom CHARMM and OPLS-AA force fields, offering computational performance improvement of at least 80%. We further use TraPPE to predict the structure and properties of LiPF(6) salt in these solvents and their mixtures. EC and PC form complete solvation shells around Li(+) ions, while the salt in DMC forms chain-like structures. In the poorest solvent, DME, LiPF(6) forms globular clusters despite DME’s higher permittivity than DMC. |
format | Online Article Text |
id | pubmed-10026065 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2023 |
publisher | American Chemical Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-100260652023-03-21 Extension of the TraPPE Force Field for Battery Electrolyte Solvents Luo, Zhifen Burrows, Stephen A. Smoukov, Stoyan K. Fan, Xiaoli Boek, Edo S. J Phys Chem B [Image: see text] Optimizing electrolyte formulations is key to improving performance of Li-/Na-ion batteries, where transport properties (diffusion coefficient, viscosity) and permittivity need to be predicted as functions of temperature, salt concentration and solvent composition. More efficient and reliable simulation models are urgently needed, owing to the high cost of experimental methods and the lack of united-atom molecular dynamics force fields validated for electrolyte solvents. Here the computationally efficient TraPPE united-atom force field is extended to be compatible with carbonate solvents, optimizing the charges and dihedral potential. Computing the properties of electrolyte solvents, ethylene carbonate (EC), propylene carbonate (PC), dimethyl carbonate (DMC), diethyl carbonate (DEC), and dimethoxyethane (DME), we observe that the average absolute errors in the density, self-diffusion coefficient, permittivity, viscosity, and surface tension are approximately 15% of the corresponding experimental values. Results compare favorably to all-atom CHARMM and OPLS-AA force fields, offering computational performance improvement of at least 80%. We further use TraPPE to predict the structure and properties of LiPF(6) salt in these solvents and their mixtures. EC and PC form complete solvation shells around Li(+) ions, while the salt in DMC forms chain-like structures. In the poorest solvent, DME, LiPF(6) forms globular clusters despite DME’s higher permittivity than DMC. American Chemical Society 2023-03-02 /pmc/articles/PMC10026065/ /pubmed/36862420 http://dx.doi.org/10.1021/acs.jpcb.2c06993 Text en © 2023 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by/4.0/Permits the broadest form of re-use including for commercial purposes, provided that author attribution and integrity are maintained (https://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Luo, Zhifen Burrows, Stephen A. Smoukov, Stoyan K. Fan, Xiaoli Boek, Edo S. Extension of the TraPPE Force Field for Battery Electrolyte Solvents |
title | Extension of the
TraPPE Force Field for Battery Electrolyte
Solvents |
title_full | Extension of the
TraPPE Force Field for Battery Electrolyte
Solvents |
title_fullStr | Extension of the
TraPPE Force Field for Battery Electrolyte
Solvents |
title_full_unstemmed | Extension of the
TraPPE Force Field for Battery Electrolyte
Solvents |
title_short | Extension of the
TraPPE Force Field for Battery Electrolyte
Solvents |
title_sort | extension of the
trappe force field for battery electrolyte
solvents |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10026065/ https://www.ncbi.nlm.nih.gov/pubmed/36862420 http://dx.doi.org/10.1021/acs.jpcb.2c06993 |
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