Page 168 - Gas Wettability of Reservoir Rock Surfaces with Porous Media
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152     Gas Wettability of Reservoir Rock Surfaces with Porous Media



                                     20,000
                                     18,000                                       82.94
                                     16,000
                                     14,000                                   74.85
                                   Resistivity, Ω.m  10,000
                                     12,000


                                      8000
                                      6000
                                                                       Gas wetting core
                                      4000
                                                                       Water wetting core
                                      2000
                                        0
                                          0        20       40       60        80       100
                                                         Gas saturation, %
                            FIGURE 4.18
                            Electrical resistance of cores with different gas saturations.


                            when there was no water flow from the rock sample, the flow pressure was
                            shut off and the rock sample was taken out for weighing and calculating the
                            gas saturation using formulae (4.10). In addition, electrical resistance of
                            the rock at 1000 HZ frequency was measured with a type TH28110B LCR
                            Puente Digital, as displayed in Fig. 4.18. The gas saturation was calculated
                            using the following formula:
                            Gas saturation 5 saturated core mass  air-blown core massÞ=pore volume
                                           ð
                                                                                           (4.10)

                            From Fig. 4.18, it can be seen that when gas saturation of cores is very low,
                            the simulated formation water is the continuous phase in pores, and electrical
                            resistance is low to moderate. When gas saturation rises and water saturation
                            decreases, the effect of wettability on core electrical resistance becomes quite
                            important. In water-wetting cores, electrical resistance is gradually increased as
                            gas saturation increases. When gas saturation exceeds 40%, unstable drops of
                            water are generated from the continuous water in the pores, breaking the con-
                            tinuity of the conduction path. Electrical resistance rapidly increases and gas
                            saturation turns into critical gas saturation. In gas-wetting cores, the change in
                            electrical resistance is similar to water-wet cores. Electrical resistance also
                            increases rapidly with the destruction of continuity of the conduction path in
                            the simulated formation water when gas saturation is about 40%.
                            From Fig. 4.18, it can be seen that the maximum gas saturation of water-
                            wetting cores is 74.85%, and the corresponding water saturation is 25.15%.
                            While the maximum gas saturation of the gas wetting cores is 82.94%, and its
                            water saturation is only 17.06%.
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