Even for such simple mixtures as (argon+methane), the excess enthalpy
H-m(E) and the excess volume V-m(E) in the near critical region are ab
out two orders of magnitude higher than for the liquid mixture at low
temperatures and pressures near ambient conditions. Mixtures for which
the critical temperatures are close together, and for which the criti
cal pressures are far apart, have similar H-m(E) (x,p,T) and V-m(E) (x
,p,T) surfaces, and near critical isotherms show double maxima in the
supercritical fluid region. Mixtures for which the critical pressures
are close together, and the critical temperatures are far apart, also
have similar H-m(E) (x,p,T) and V-m(E) (x,p,T) surfaces, but isobars o
n the surfaces are 'S' shaped. The shapes of these near-critical exces
s-function surfaces can be understood from an inspection of the enthal
py, or residual enthalpy curves of the mixture and of the pure compone
nts. Examples of both are given. Attention is drawn to the large value
that these excess functions can have close to a pure component critic
al point. (C) 1997 Elsevier Science B.V.