For internal energy relaxation in rarefied gas mixtures, exact relatio
nships are derived between the selection probability P employed in dir
ect simulation Monte Carlo (DSMC) methods and the macroscopic relaxati
on rates dictated by collision number Z in Jeans' equation. These expr
essions apply to the Borgnakke-Larsen model for internal energy exchan
ge mechanics and are not limited to the assumption of constant Z. Alth
ough Jeans' equation leads to adiabatic relaxation curves, which coale
sce to a single solution when plotted against the cumulative number of
collisions, it is shown that the Borgnakke-Larsen selection probabili
ties depend upon the intermolecular potential, the number of internal
degrees of freedom, and the DSMC selection methodology. Furthermore, s
imulation results show that the common assumption P = 1/Z is invalid,
in general, and leads to considerably slower relaxation than stipulate
d by Z in Jeans' equation. Moreover, inconsistent definitions of colli
sion rates appearing in the literature can lead to considerable errors
in DSMC models. Finally, for general gas mixtures, Borgnakke-Larsen D
SMC kinetics match Jeans' behavior exactly only when using a selection
methodology, which prohibits multiple relaxation events during a sing
le collision.