Page 167 - Gas Wettability of Reservoir Rock Surfaces with Porous Media
P. 167

Effect of Gas Wettability on the Surface Properties CHAPTER 4                       151



                        3000

                        2500                            Water wetting core
                                                        Gas wetting core
                      Resistivity, Ω.m  1500
                        2000





                        1000

                        500
                            0       200      400      600     800      1000
                                             Frequency, KHZ
              FIGURE 4.17
              Electrical resistance changes in cores with different wettabilities in saturated simulation formation water.



              using a wet filter paper, which was drenched with water from the formation
              layer until there were no obvious reflected light. The core was placed in a core
              holder to conduct an electrode sweep frequency measurement of the saturated
              cores. The frequency ranged from 100HZ to 1MHZ and 100 200 points were
              taken. The electrical resistance changes in cores before and after gas-wetting
              alteration in saturated simulation formation water are displayed in Fig. 4.17.

              4.3.1.2.2   Electrical resistance of cores with different
              wettabilities in saturated simulation formation water
              From Fig. 4.17, it can be seen that when the water-wetting cores and gas-
              wetting cores are saturated with the simulated formation water, their measured
              electrical resistances are the same. They decrease as the frequency increases,
              and there is little difference in values. It is thus clear that the main component
              for conducting current is the continuous water in the connecting pores under
              high water saturation. At this time, electrical resistance mainly depends on the
              mineralization of the simulated formation water and the structure of core
              pores. Thus, there is little difference between electrical resistance of water-
              wetting cores and gas-wetting cores under high water saturation.

              4.3.2   Relationship Between Gas Saturation and Electrical
              Resistance of Rocks
              4.3.2.1 ELECTRICAL RESISTANCE OF CORES UNDER DIFFERENT
              SATURATIONS
              For cores with different wettabilities that were saturated with simulated forma-
              tion water, a fully-automatic gas permeability meter JHGP was used to
              increase gradually the flowing pressure from low to high, and an experimental
              confining pressure p and temperature T was imposed. In every pressure spot,
   162   163   164   165   166   167   168   169   170   171   172