In this communication we review the bases for a collection of equation
of state mixing rules which have been developed that combine activity
coefficient (or excess free energy of mixing)models with equations of
state. We show that combining equations of state and activity coeffic
ient models at infinite pressure produces mixing rules that are free o
f ad hoc assumptions, and are easy to understand and implement. In con
trast, when the link is made at zero or low pressure, problems arise b
ecause the liquid volume appears in the mixing rule. In principle, thi
s requires solving the equation of state for the liquid volumes of eac
h of the pure components and for the mixture. To avoid such calculatio
ns, and to deal with the problem that a liquid phase solution to the e
quation of state may not exist for one or more of the pure components
at the temperature of interest, several ad hoc procedures have been pr
oposed. It is these procedures that differentiate between the various
zero (low) pressure mixing rules. Each of the mixing rules reviewed he
re is successful for at least some range of temperatures, though some
of their shortcomings are discussed. Finally, two new variants of this
class of mixing rules are proposed, of which one is tested and found
to be simple, and at least as satisfactory as presently used zero-pres
sure mixing rules.