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Viscosities of triethyloctylphosphonium bis(trifluoromethanesulfonyl)amide, P222,8Tf2N, are reported as a function of temperature (273 to 363) K and pressure (maximum 302 MPa) with a falling-body viscometer together with electrical conductivities (κ) measured by impedance spectroscopy at (283 to 348) K, to 250 MPa maximum pressure. pVT data were determined with a vibrating tube densimeter from (298 to 353) K to 50 MPa. Ion self-diffusion coefficients (DSi) were measured by steady-gradient spin-echo NMR (313 to 365) K, and densities (273 to 363) K were determined with a vibrating tube densimeter, both at atmospheric pressure. The results were correlated with Walden and Stokes–Einstein–Sutherland relations. Velocity cross-correlation coefficients (VCC), distinct diffusion coefficients (DDC) and Laity resistance coefficients (LRC) were calculated from DSi and κ at 0.1 MPa. The DDC and LRC for P222,8Tf2N and the pentyl-substituted analogue, P222,5Tf2N, showed differences for cation–cation and cation–anion velocity anti correlations, presumably due to the different cation structures. The high-pressure viscosities were used to predict the pressure dependence of the glass-transition temperature for P222,5Tf2N and P222,8Tf2N. Density scaling was applied to the high-pressure viscosities and conductivities of P222,8Tf2N for comparison with P222,5Tf2N. The scaling parameters are consistent with the theoretical treatment of Knudsen et al. for ionic liquids.
Harris et al. (Thu,) studied this question.
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