Some of the properties of gas phase relaxation and transport are revie
wed with an emphasis on those properties that are due entirely to the
presence of internal states in real molecular systems. The theoretical
formulations of such non-equilibrium effects is based on the quantum
Boltzmann equation. The conditions for the validity and the properties
of this equation are reviewed. This includes a general discussion of
how the combination of free molecule motion and collisions is required
for the approach to global equilibrium. It is shown how the free moti
on is equivalent to a phase randomization of the elements of the densi
ty operator that are off-diagonal in energy. Spin relaxation and the m
agnetic held dependence (Senftleben-Beenakker effects) of the viscosit
y for a gas of diatomics are used to illustrate these aspects of the a
pproach to equilibrium.