Experiments have been carried out to study the displacement of wetting flui
ds by immiscible non-wetting fluids in quasi-two-dimensional and three-dime
nsional granular porous media. These experiments included a systematic inve
stigation of the effects of gravity acting on the density difference betwee
n the two fluids. The simple invasion percolation model provides a surprisi
ngly realistic simulation of the slow fluid fluid displacement process in t
he absence of gravity, and a simple extension of the model can be used to s
imulate the most important features of gravity stabilized and destabilized
fluid-fluid displacement processes. The dimensionless Bond number Bo (the r
atio between buoyancy forces and capillary forces on the pore scale) can be
used to compare experiments and simulations carried out using different (g
eometrically similar) porous media, different fluid-fluid interfacial tensi
ons and different fluid densities. The complex patterns generated by gravit
y stabilized and gravity destabilized fluid fluid displacement processes ca
n be described in terms of a pattern of blobs of size xi that have a fracta
l structure on length scales l in the range c less than or equal to l less
than or equal to xi, where c is the characteristic porous medium grain size
. The blob size xi is related to the Bond number by the simple scaling rela
tionship xi similar to Bo(-v/(1+v)), which was first derived by Wilkinson (
1984, 1986) for gravity-stabilized displacement. Here, v is the percolation
theory correlation length exponent (v=4/3 in two-dimensional systems and v
approximate to 0.88 in three-dimensional systems). The experiments and sim
ulations have been extended to include fluid-fluid displacement in fracture
apertures and the effects of how of the wetting fluid under the influence
of a hydraulic potential gradient. These experimental and simulation result
s have important implications for our understanding of secondary migration.
They indicate that the residual hydrocarbon saturation in the enormous vol
ume of porous sedimentary rock (carrier rocks) between the hydrocarbon sour
ce and the reservoir can be very low, thus allowing significant quantities
of oil and gas to reach the reservoir. Simulations have been carried out to
explore the effects of heterogeneities on gravity destabilized fluid-fluid
displacement processes and fluid fluid displacement in fracture apertures.
However, the structure of the carrier rocks is highly dynamic on the time
scales over which secondary migration takes place (of the order of 10(8) ye
ars, in many cases). A better understanding of the pore structure of the ca
rrier rocks and its dynamics on long time scales is needed to more accurate
ly model secondary migration. (C) 2000 Elsevier Science Ltd. All rights res
erved.