It has been noted previously that Hele-Shaw (parallel-plate) models are better than other types of laboratory models to properly scale down miscible displacements from field size to laboratory size. In most miscible flooding processes, however, the miscible displacement is preceded or followed by an immiscible displacement in which oil or gas is trapped by water, or waterflood residual oil is reconnected by a miscible slug. This trapping and reconnection could not be simulated in a conventional parallel-plate model. parallel-plate model. Now, however, a new version of this type of model has been invented that simulates the trapping behavior of porous rock. Instead of trapping by capillary (surface tension) forces, the new model traps light fluids by density difference (Fig. 1). A model of this type can be used to simulate, for example, the tertiary recovery process in which a solvent slug (e.g., CO2) injected in a waterflooded oil field and then followed by another water drive. The particular model devised for this purpose was made of 3-in. thick, 14-in. square plates purpose was made of 3-in. thick, 14-in. square plates of Plexiglas. The top plate contained 596 pairs of 1/40-in.-diameter holes, 112 in. apart at the base, and meeting 3/4 in. deep in the plate. Vent holes 1/16in. in diameter were drilled from the other side of the plate to the junctions of these pairs. The 12- x 12-in. square perforated region was supplied with wells in a nine-spot pattern, and was sealed around the periphery by an O-ring in a rectangular groove. The plates were held a fixed distance apart by shims and bolts outside the O-ring. A typical plate spacing was 0.01 cm. After the model was filled with liquids and air was forced out of the trapping holes, the vent holes were plugged with rods. P. 255