The self-diffusion coefficient (D) of liquid CS2 has been determined by com
puter simulation for seven densities (rho) and eight temperatures, spanning
more than two decades of D in the supercooled and near-melting normal liqu
id, and bracketing the P=1 atm isobar. Super-Arrhenius behavior of -log D v
s 1/T, an increase in slope with decreasing T, is found at 1 atm, but norma
l Arrhenius T dependence holds along all seven different isochores, even at
the highest density and lowest T. The super-Arrhenius behavior is a conseq
uence of the variation in density rho(T) at constant pressure. Physically m
eaningful activation energies, representative of the heights of the barrier
s to diffusion, depend upon rho only, are smaller than the isobaric slope,
and may be obtained by correcting it or from an Arrhenius plot at constant
density. Barriers to diffusion are indeed higher at lower temperatures, but
only due to the higher density. The importance of T vs rho as the "control
variable" for diffusion is examined. Temperature and density play comparab
le roles near the melting states, and the relative importance of T grows wi
th supercooling. However that growth is due to the higher activation energy
, itself controlled by density. (C) 1999 American Institute of Physics. [S0
021-9606(99)51422-0].