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Sahimi et al.
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                             To control the mobility, many different methods have been used, such as
                           water-alternating-gas (WAG), gas-soluble viscofiers, gelled and cross-linked poly-
                           mers, and surfactants and foams (Smith, 1988). We describe one of these, namely,
                           the WAG process.
                           8.10.3  Miscible Water-Alternative-Gas Process

                           This method is the only gas-flood mobility control technique which is used regularly
                           in field applications. Its chief virtues are familiarity to the petroleum engineers, as
                           it consists of the familiar water flooding, alternated with gas flooding; simplicity,
                           having timing and the ratio of water to gas as its only design parameters, and its low
                           cost. It is used mostly to maintain pressure while the solvent supply is interrupted, or
                           to stretch out injection costs by substituting water for the more expensive solvent.
                             Miscible WAG injection has been implemented successfully in a number of fields
                           around the world (Christensen et al. 1998a,b). In principle, it combines the benefits
                           of miscible gas injection and water flooding by injecting the two fluids either simul-
                           taneously or alternatively. Miscible gas injection has excellent microscopic sweep
                           efficiency, but poor macroscopic sweep efficiency due to fingering and gravity over-
                           ride. Furthermore, it is expensive to implement. The optimal ratio for simultaneous
                           WAG injection in a relatively homogeneous reservoir can be estimated by matching
                           the advance rates of the water-oil and solvent-oil displacement fronts. Water flooding,
                           on the other hand, is cheaper and less vulnerable to gravity segregation and frontal
                           instabilities. However, the residual oil saturations after water flooding are relatively
                           high.
                             Johns et al. (2003) studied optimization of the WAG processes for enriched gas
                           floods, particularly as a primary recovery method. Al-Shuraiqi et al. (2003) carried
                           out laboratory investigations of first-contact miscible WAG to study the effects of
                           WAG ratio and flow rate on recovery efficiency. Their experiments (using bead-
                           packs) indicated that, (1) recovery from WAG may vary with rate, even when gravity
                           is neglected, and (2) water-solvent and water-oil relative permeabilities may not be
                           the same if they are first-contact miscible. The influence of the rate on WAG recovery
                           appearstobeduetotherate-dependencyofwater-oilandwater-solventpermeabilities.

                           8.10.4  Relative Permeabilities

                           Enhanced oil recovery processes that are carried out under near miscible conditions
                           require relative permeability data to calculate the flow behavior of the low interfa-
                           cial tension (IFT) fluids. In systems where the displacing and displaced fluids are
                           miscible and the flow velocity is low enough that the process is controlled by diffu-
                                                                        ◦
                           sion, the fractional flow versus saturation curve is a 45 line, and is referred to as
                           miscible relative permeability function. The term near-miscible relative permeability
                           functions is used to denote the curves found in the region between the immiscible
                           limit and miscible limits. If the IFT is finite and there is no mass transfer, the relative
                           permeabilities of the phases are, as is well-known, more complicated.
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