Thermodynamic, structural and dynamic properties of ionic liquids C(4)mimCF3COO, C(4)mimBr in the condensed phase, using molecular simulations
J Sanchez-Badillo and M Gallo and RA Guirado-Lopez and J Lopez-Lemus, RSC ADVANCES, 9, 13677-13695 (2019).
DOI: 10.1039/c9ra02058f
In this work a series of thermodynamic, structural, and dynamical properties for the 1-butyl-3-methylimidazolium trifluoroacetate (C(4)mimCF3COO) and 1-butyl-3-methylimidazolium bromide, (C(4)mimBr) ionic liquids (ILs) were calculated using Non- polarizable Force Fields (FF), parameterized using a methodology developed previously within the research group, for condensed phase applications. Properties such as the Vapor-Liquid Equilibrium (VLE) curve, critical points (rho(c), T-c), Radial, Spatial and Combined Distribution Functions and self-diffusion coefficients were calculated using Equilibrium Molecular Dynamics simulations (EMD); other properties such as shear viscosities and thermal conductivities were calculated using Non-Equilibrium Molecular Dynamics simulations (NEMD). The results obtained in this work indicated that the calculated critical points are comparable with those available in the literature. The calculated structural information for these two ILs indicated that the anions interact mainly with hydrogen atoms from both the imidazolium ring and the methyl chain; the bromide anion displays twice the hydrogen coordination number than the oxygen atoms from the trifluoroacetate anion. Furthermore, Non-Covalent interactions (NCI index), determined by DFT calculations, revealed that some hydrogen bonds in the C(4)mimBr IL displayed similar strength to those in the C(4)mimCF3COO IL, in spite of the shorter O--H distances found in the latter IL. The majority of the calculated transport properties presented reasonable agreement with the experimental available data. Nonetheless, the self-diffusion coefficients determined in this work are under-estimated with respect to experimental values; however, by escalating the electrostatic atomic charges for the anion and cation to +/- 0.8e, only for this property, a remarkable improvement was obtained. Experimental evidence was recovered for most of the calculated properties and to the best of our knowledge, some new predictions were done mainly in thermodynamic states where data are not available. To validate the FF, developed previously within the research group, dynamic properties were also evaluated for a series of ILs such as C(4)mimPF6, C(4)mimBF4, C(4)mimOMs, and C(4)mimNTf2 ILs.
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