Page 84 - Gas Wettability of Reservoir Rock Surfaces with Porous Media
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68      Gas Wettability of Reservoir Rock Surfaces with Porous Media



                            The dispersion part, polarity part, and free energy of solid surface can be
                            obtained from Eqs. (2.43) and (2.44), which is as follows:

                            γ d SV  5  466:56 1 1090:8cosθ Oct 2 1557:36cosθ Air           (2.45)
                                     64:8 2 50:5cosθ Oct 1 72:1cosθ Air
                            γ p  5  2550:25ð1 2 cosθ Oct Þ                                 (2.46)
                             SV
                                  151:5 1 50:5cosθ Oct
                            γ SV  5 γ d SV  1 γ p SV  5  466:56 1 1090:8cosθ Oct 2 1557:36cosθ Air
                                                64:8 2 50:5cosθ Oct 1 72:1cosθ Air
                                                                                           (2.47)
                                              2550:25ð1 2 cosθ Oct Þ
                                            1
                                              151:5 1 50:5cosθ Oct
                            Solid/water interface free energy γ SW  and solid/n-octane interface free energy
                            γ SO  can be obtained by using the free energy of solid surface calculated from
                            Eqs. (2.45) (2.47), and the dispersion and polarity parts of free energy in
                            Eqs. (2.39) and (2.40). At the same time, from Eqs. (3.28) and (3.29), it can
                            be seen that only the dispersion part γ d SV  of solid surface energy is related to
                            the contact angle θ Air of air bubbles on solid/water interface, and the disper-
                            sion and polarity parts are not mutually independent. As jointly determined
                            by the solid surface energy γ , contact angle of air bubbles θ Air and contact
                                                      SV
                            angle of n-octane liquid drops θ Oct .
                               2. Theoretical study of the effects of free energy of liquid surface and solid/liquid
                                 interface free energy on gas wettability
                                    In the gas-liquid-solid system, the captive bubble method is commonly
                                 used for measuring solid/liquid interface free energy and surface free
                                 energy of liquid. It is extensively used in the medical field [35,36].The
                                 contact angle of the liquid in bubble capture method is the measured
                                 receding angle ðθ R Þ when solid/liquid interface decreases and is replaced
                                 by solid/gas interface, as displayed in Fig. 2.30. The greater the θ R ,the
                                 stronger the capability of gas displacing liquid on a solid surface.
                                 Therefore the contact angle of gas on solid/liquid interface ðθ G Þ is regarded
                                 as representing wettability of the solid/liquid interface due to gas.















          FIGURE 2.30
          Schematic diagram of bubble capture method (air bubble).
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