It is generally accepted that the reservoir depletion process is a dif
ferential liberation process where the eas is removed from contact wit
h the oil as soon as it is formed, and the production of I fluids thro
ugh tubing and separators is a flash liberation process where the gas
liberated from solution remains in contact with the oil. Laboratories
commonly perform differential liberation and separator tests on the re
servoir fluid and then use a correlation described by Amyx et al.((1))
to arrive at a composite liberation curve for an optimum separator pr
essure. Engineers are often confused as to which of the two sets of PV
T data, i.e., differential or composite, should be used in a black oil
simulation of the reservoir. The differences between the two sets of
data become more substantial as the API gravity of the oil increases.
The black oil simulator used in this report has a compositional formul
ation and has the ability to rigorously model the PVT behaviour by ent
ering differential liberation data for reservoir conditions and using
a surface separator option for the surface Bash process. This paper de
scribes a critical comparison of the three methods to enter PVT proper
ties in a black oil simulator, The results of using the simulator in t
hree ways: a) differential liberation at reservoir, surface separator
for flash, b) composite liberation data, c) differential liberation da
ta, are described in this paper for a medium gravity crude. It is show
n that the composite liberation data most closely represents the rigor
ous representation of phase behaviour as in (a). Use of inappropriate
liberation data could results in significant error in estimates of oil
-in-place as in (c). The paper compares the differences between compos
ite liberation (b) and the rigorous representation (a), such as differ
ent initial pressure and saturation gradients due to initial density d
ifferences.