A systematic study of the self-diffusion coefficient inhard-sphere fluids, Lennard-Jones fluids,and real compounds over the entire range of gaseous and liquid statesis presented. First anequation is proposed for the self-diffusion coefficient in ahard-sphere fluid based on the moleculardynamics simulations of Alder et al. (
J. Chem. Phys.1970,
53, 3813) and Erpenbeck andWood(
Phys. Rev. A 1991,
43, 4254).That expression, extended to the Lennard-Jones fluidsthroughthe effective hard-sphere diameter method, represents accurately theself-diffusion coefficientsobt
ained in the literature by molecular dynamics simulations, as wellas those determinedexperimentally for argon, methane, and carbon dioxide. A roughLennard-Jones expression,which cont
ains besides the diameter
LJ and energy
LJ the translational-rotational factor,
AD(which could be correlated with the acentric factor), is adopted todescribe the self-diffusion innonspherical fluids. The energy parameter is estimated using acorrelation obt
ained fromviscosity data, and the molecular diameter is obt
ained from thediffusion data themselves. Theequation represents the self-diffusion coefficients with an averageabsolute deviation of 7.33%,for 26 compounds (1822 data points) over wide ranges of temperature andpressure.