Knowledge of the fluid-fluid and fluid-solid interfacial areas is impo
rtant to better understand and quantify many flow and transport proces
ses in porous media. This paper presents estimates for interfacial are
as of porous media containing two or three fluids from measured capill
ary pressure (P-c)-saturation (S) relations. The thermodynamic treatme
nt of two-fluid P-c-S relations presented by Morrow (1970) served as t
he basis for the predictions. In media containing two fluids (air-oil,
air-water, oil-water), the solid-nonwetting interfacial area (A(sN))
equaled zero when the solid was completely wetted by the wetting flui
d. The area under the P-c-S curve was directly proportional to the non
wetting-wetting interfacial area (A(NW)). If the solid surface was no
t completely wetted by one fluid, A(NW) and A(sN)* were estimated by
weighed partitioning of the area under the P-c-S curve. For porous med
ia with fractional wettability, the procedure was applied separately t
o water- and oil-wet regions. The values of A(NW) and A(sN)* were hig
hest and lowest, respectively, in systems that were strongly wetted. I
n three-fluid media the wetting and spreading behavior of the liquids
greatly affected the estimated interfacial areas. For a water-wet medi
um with a continuous intermediate oil phase, the interfacial areas wer
e predicted from P-c-S data in a similar manner as for two-fluid media
. The oil-water and oil-solid interfacial areas were estimated from th
e oil-water P-c-S curve, while the air-oil interfacial area was obtain
ed from the air-oil P-c-S curve. For a fractional wettability or oil-w
et medium there may be as many as six interfaces. These interfacial ar
eas were estimated from three-fluid P-c-S relations based on previousl
y developed methods for predicting three-fluid P-c-S relations from tw
o-fluid data. (C) 1997 Elsevier Science B.V.