Wa. Van Hook et al., An interpretation of the vapor phase second virial coefficient isotope effect: Correlation of virial coefficient and vapor pressure isotope effects, J PHYS CH A, 105(40), 2001, pp. 9284-9297
Experimental data on vapor phase second virial coefficient isotope effects
(VCIEs) are reviewed and then interpreted using the general theory of isoto
pe effects. Useful correlations are developed between -Delta (B - b(o))(B -
b(o)) = (-VCIE) and [ln(f(c)/f(g))]*, where [ln(f(c)/f(g))]* is the refere
nce condensed phase reduced isotopic partition function ratio, and A is the
second virial coefficient, b(o) = 2 pi sigma (3)/3. sigma is the Lennard-J
ones size parameter, and Delta denotes an isotopic difference, light-heavy.
[ln(f(c)/f(g))]* can be straightforwardly obtained from measurements of va
por pressure isotope effects for T-R = T/T-CRITICAL < 0.7. We show (-VCIE)
= ln(f(p)/f(g)(2)) where ln(f(p)/f(g)(2)) is the reduced isotopic partition
function ratio associated with the equilibrium between isolated gas-phase
monomer species and interacting pairs. At temperatures well removed from cr
ossovers in ln(f(p)/f(g)(2)) or [ln(f(c)/f(g))]*, ln(f(p)/f(g)(2)) = (0.4 /- 0.2) [ln(f(c)/f(g))]*.