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84                                                   MULTIPHASE FLOW
              IFT has units of force per unit length, which is equivalent to energy per unit area.
           IFT can refer to the force acting at the boundary of the interface between two phases or
           to the energy needed to form the area within the boundary. IFT arises because of the
           differences in molecular attractions that are experienced by molecules at the interface
           between phases. Consider, for example, a water–oil interface. In water, molecules are
           capable of hydrogen bonding with each other because of their polarity and shape. In
           oil, molecules have little or no polarity, and bonding between molecules is weak. A
           water molecule at the interface will feel strong attractive forces toward the other water
           molecules in the water phase but not from the molecules in the oil phase. This difference
           in attractions produces IFT. Some examples of IFT are listed in Table 5.1.
              An important consequence of IFT is a difference in pressure between two adjacent
           phases. That pressure difference is called capillary pressure p . It is proportional to
                                                             c
           IFT and the inverse of curvature of the interface. For a spherical oil drop of radius r
           surrounded by water, capillary pressure is the difference in pressure given by
                                                  2σ
                                    p   =  p − p =  ow                     (5.1)
                                     cow  o   w    r
           where σ  is the oil–water IFT. Pressure inside the drop of oil is higher than pressure
                  ow
           in the surrounding water. Capillary pressure increases with decreasing size of pore
           space. Shales have very small pores and capillary pressure can approach 1000 psi.
              Wettability is a result of the interactions between a solid surface and two adjacent
           fluid phases as shown in Figure  5.1. The contact angle is the most fundamental
             measure  of  wettability.  Figure  5.1a  shows  water  and  oil  in  contact  with  a  solid
             surface. The surface is termed water wet because the contact angle is less than 90°.
           In this competition for contact with the solid, the water is spreading over the solid.
           Water is the wetting phase and oil is the nonwetting phase. If a droplet of water is
           placed on a clean glass surface with surrounding air, its shape is similar to

                           TABLE 5.1  Examples of Interfacial Tension
                           Fluid Pair  IFT Range (mN/m or dyne/cm)
                           Air–brine           72–100
                           Oil–brine           15–40
                           Gas–oil             35–65


                (a)                               (b)
                                                                   Contact
                                                                   angle,
                                 Contact
                                 angle,
                   Oil                               Oil
                         Water                              Water
                              Solid                              Solid
                        Water wet                          Oil wet

           FIgURE  5.1  Wettability of  a surface  in contact with two  phases is measured by the
           contact angle.
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