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The aim of this work is to understand the details of the interactions of ionic liquids with carbon nanomaterials (graphene and nanotubes) using polyaromatic compounds as model solutes. We have combined the measurements of thermodynamic quantities of solvation with molecular dynamics simulations to provide a microscopic view. The solubility of five polycyclic aromatic hydrocarbons (naphthalene, anthracene, phenanthrene, pyrene and coronene) was determined in seven ionic liquids ([C4C1im][C(CN)3], [C4C1pyrr][Ntf2], [C10C1im][Ntf2], [C2C1im][C(CN)3], [C2C1im][Ntf2], [C3C1pyrr][N(CN)2] and [C4C1im][N(CN)2]) at 298 K. The enthalpies of the dissolution of naphthalene, anthracene and pyrene were measured in four of the ionic liquids. Free energies were estimated from those measurements in order to analyse the entropic or enthalpic contributions to the dissolution process. Molecular dynamics simulations provided solvation free energies that were compared to experimental and structural information. Spatial distributions of solvent ions around the solutes when combined with IR measurements elucidate the structure of solvation environments. Interactions between the imidazolium rings of cations and the π system of the solutes have been identified. However, ionic liquids with pyrrolidinium cations appeared as better solvents due to favourable enthalpic contributions compared to imidazolium cations. Long alkyl side chains on cations lead to higher solubility and lower enthalpy of dissolution by creating a “softer” solvation environment. Considering the effect of anions, small and planar anions lead to higher solubilities and lower enthalpies of dissolution of polyaromatic hydrocarbons. These findings provide the design principles based on molecular interactions and the structure of solvation environments to choose or formulate ionic liquids in view of their affinity for carbon nanomaterials. [ABSTRACT FROM AUTHOR]

Classical molecular dynamics (MD) simulation of OH in liquid water at 37 °C has been performed using flexible models of the solute and solvent molecules. We derived the Morse function describing the bond stretching of the radical and the potential for OH–H2O interactions, including short-range interactions of hydrogen atoms. Scans of the potential energy surface of the OH–H2O complex have been performed using the DFT method with the B3LYP functional and the 6-311G(d,p) basis set. The DFT-derived partial charges, ±0.375e, and the equilibrium bond-length, 0.975 Å, of OH resulted in the dipole moment of 1.76 D. The radical–water radial distribution functions revealed that OH is not built into the solvent structure but it rather occupies distortions or cavities in the hydrogen-bonded network. The solvent structure at 37 °C has been found to be the same as that of pure water. The hydration cage of the radical comprises 13–14 water molecules. The estimated hydration enthalpy −42 ± 5 kJ mol−1is comparable with the experimental value −39 ± 6 kJ mol−1for 25 °C. Inspection of hydrogen bonds showed the importance of short-range interaction of hydrogen atoms and indicated that neglect of the angular condition greatly overestimates the number of the H-acceptor radical-water bonds. The mean number n= 0.85 of radical-water H-bonds has been calculated using geometric definition of H-bond and n= 0.62 has been obtained when the energetic condition, Eda≤ −8 kJ mol−1, was additionally considered. The continuous lifetimes of 0.033 ps and 0.024 ps have been estimated for the radical H-donor and the H-acceptor bonds, respectively. Within statistical uncertainty the radical self-diffusion coefficient, (2.9 ± 0.6) × 10−9m2s−1, is the same as (3.1 ± 0.5) × 10−9m2s−1calculated for water in solution and in pure solvent. To the best of our knowledge, this is the first study of the OHaqproperties at a biologically relevant body temperature. [ABSTRACT FROM AUTHOR]