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276                                                          APPENDIX A

             The wettability is calculated on the basis of core sample weights measured at various
           testing modes. For example, the forced displacement of oil to S or and water to S iw may
           be conducted using a centrifuge or by mounting the core in fluid-flow equipment and
           pumping the displacing fluids into the core (see, e.g., Tiab and Donaldson, 2004, for
           details, pp. 371–373).
             Wettability may be defined also as the ability of the liquid to ‘‘wet,’’ or spread
           over, a solid surface. Fig. A.1A shows a liquid wetting a solid surface, whereas
           Fig. A.1B shows the relationship between the liquid and solid when the liquid has
           little affinity for the solid. In Fig. A.1C, the liquid drop occupies an intermediate
           position. The fluid, which wets the surface more strongly, occupies the smaller pores
           and minute interstices in a rock.
             The angle, which the liquid interface makes with the solid, is called the contact
           angle, y. Usually, it is measured from the solid through the liquid phase (if the other
           phase is a gas) and through the water phase if oil and water are both present. In a
           capillary tube, shown in Fig. A.2A, the angle between the tube wall and the tangent
           to the curved interface (where it intersects the tube wall) is less than 901. For a
           capillary depression, shown in Fig. A.2B, the contact angle is greater than 901. In the
           case of no rise or depression, the angle is 901 (see Fig. A.2C)
             Molecular interaction caused by the molecular property (intermolecular cohesive
           forces) of liquids is called the interfacial tension, y. It has the dimensions of force per
                                                                2
           unit length (lb/ft or dyn/cm) or energy per unit area (erg/cm ). Interfacial tension
           causes the curved surface of the interface between two immiscible fluid phases
           (e.g., between the gas and liquid or between two liquids, as well as the interface
           between a liquid and a solid) to contract into the smallest possible area per unit of













                           Fig. A.1. Different degrees of wetting of solid by liquid.













           Fig. A.2. Behavior of various fluids in glass capillary tubes. (a)– water, (b)– mercury, and (c)–
           tetrahydronaphtalene (when glass is perfectly clean and liquid is pure).
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