4.7 Article

Fine-Tuning the Polarizable CL&Pol Force Field for the Deep Eutectic Solvent Ethaline

期刊

JOURNAL OF CHEMICAL INFORMATION AND MODELING
卷 61, 期 12, 页码 5938-5947

出版社

AMER CHEMICAL SOC
DOI: 10.1021/acs.jcim.1c01181

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资金

  1. FAPESP (The Sao Paulo Research Foundation) [2020/06766-9, 2016/21070-5]
  2. Ministry of Education and Science of the Russian Federation [075-15-2021-954]
  3. Fundacao de Amparo a Pesquisa do Estado de Sao Paulo (FAPESP) [16/21070-5] Funding Source: FAPESP

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Polarizable force fields are becoming popular for simulations of ionic soft matter, but may face issues such as unbalanced atomic diameter parameters and overpolarization of chlorides. Corrections can be made by adjusting radial distribution functions and extending damping functions.
Polarizable force fields are gradually becoming a common choice for ionic soft matter, in particular, for molecular dynamics (MD) simulations of ionic liquids (ILs) and deep eutectic solvents (DESs). The CL&Pol force field introduced in 2019 is the first general, transferable, and polarizable force field for MD simulations of different types of DESs. The original formulation contains, however, some problems that appear in simulations of ethaline and may also have a broader impact. First, the originally proposed atomic diameter parameters are unbalanced, resulting in too weak interactions between the chlorides and the hydroxyl groups of the ethylene glycol molecules. This, in turn, causes an artificial phase separation in long simulations. Second, there is an overpolarization of chlorides due to strong induced dipoles that give rise to the presence of peaks and antipeaks at very low q-vector values (2.4 nm(-1)) in the partial components of the structure factors. In physical terms, this is equivalent to overestimated spatial nanoscale heterogeneity. To correct these problems, we adjusted the chloride-hydroxyl radial distribution functions against ab initio data and then extended the use of the Tang-Toennis damping function for the chlorides' induced dipoles. These adjustments correct the problems without losing the robustness of the CL&Pol force field. The results were also compared with the nonpolarizable version, the CL&P force field. We expect that the corrections will facilitate reliable use of the CL&Pol force field for other types of DESs.

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