Viscosities of triethyloctylphosphonium bis(trifluoromethanesulfonyl)amide,
[P222,8][Tf2N], 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 (D
Si) 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 D
Si and κ at
0.1 MPa. The DDC and LRC for [P222,8][Tf2N]
and the pentyl-substituted analogue, [P222,5][Tf2N], 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 [P222,5][Tf2N] and [P222,8][Tf2N]. Density scaling was applied to the high-pressure viscosities
and conductivities of [P222,8][Tf2N] for comparison
with [P222,5][Tf2N]. The scaling parameters
are consistent with the theoretical treatment of Knudsen et al. for
ionic liquids.