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72      Gas Wettability of Reservoir Rock Surfaces with Porous Media




                                                 ζ gas-water  in air, gas wettability index of gas on the
                                                 surface of glass slide with respect to water
                          0.3

                          0.2

                         ζ gas-water  0.1

                          0.0
                            –25  –20   –15  –10   –5   0     5    10   15

                          –0.2      A  Work of adhesion (mJ/m )
                                                     2
                                     W
                          –0.2

          FIGURE 2.33
                                              W
          Relationship between ζ gas-water and work of adhesion A .


                                                                                  W
                            Figs. 2.32 and 2.33 show: (1) whenγ glass slide ,γ glass slide-water , A , 0, air prefer-
                            entially wets the surface of glass slide with respect to water, with gas-wetting
                                                                                 W
                            parameter ζ gas-water .0. (2) when γ glass slide . γ glass slide-water ,A . 0, air doesn’t
                            preferentially wet the surface of glass slide with respect to water, with gas-
                            wetting parameter ζ gas-water ,0. (3) with increasing γ glass slide-water and decreas-
                            ing γ glass slider ,i.e., as A W  gradually reduces, wettability of glass slide surface
                            caused by air with respect to water is enhanced. When γ glass slide 5 γ glass slide-water ,
                             W
                            A 5 0, the glass slide surface shows intermediate-wetting capacity, as wetting is
                            the process by which solid free energy is decreased according to the laws of ther-
                            modynamics. Thus when the glass slide/air interface free energy is less than
                            glass slide/water interface free energy, air preferentially wets the surface of glass
                            slide. Work of adhesion represents the capability of water to replace air on the
                            glass slide surface. Therefore as A W  decreases, ζ gas-water increases, i.e., gas wetta-
                            bility is enhanced.

                            In glass slide-n-hexadecane system, the relationship between gas-wetting
                            parameter ζ gas-inn-hexadecane of glass slide surface caused by air with respect to
                            n-hexadecane, and glass slide/n-hexadecane interface free energy γ glass slide-inn-
                            hexadecane and free energy of glass slide surface γ glass slide is displayed in
                            Fig. 2.34. The relationship between ζ gas- inn-hexadecane and the work of adhesion
                            A Hex  is displayed in Fig. 2.35.

                            Figs. 2.34 and 2.35 show that within the experimental range, when γ glass slide
                            .γ glass slide-hexadecanehas , A Hex  . 0, ζ gas-hexadecanehas , 0, the gas is in nonwetting
                            phase. As the work of adhesion A Hex  increases, ζ gas-hexadecanehas decreases and gas
                            wettability weakens, which is because when γ glass slide ,γ glass slide-hexadecanehas
                            compared with air, n-hexadecane has greater capacity to lower the surface energy
                            of the glass slide. A Hex  . 0 indicates that n-hexadecane has stronger capacity to
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