Page 281 - Enhanced Oil Recovery in Shale and Tight Reservoirs
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258                            Enhanced Oil Recovery in Shale and Tight Reservoirs


             The relationship among the transverse relaxation time T 2 in porous me-
          dia, the transverse relaxation time of the bulk liquid T 2,bulk , the surface area
          A of the pore, the surface relativity r, and the volume of the pore is (Looyes-
          tijn and Hofman, 2006)
                                   1     1       A
                                     ¼       þ r                     (9.44)
                                  T 2  T 2;bulk  V
             The effect of fluid diffusion (DGT E g/12) can be added in the above
                                                      2
          equation, D is the fluid diffusion coefficient (cm /s), G is the magnetic
          gradient, T E is the echo spacing of measurement sequence (ms), and g is
          the gyromagnetic ratio. In the experiment conditions where the magnetic-
          field of the NMR apparatus is relatively uniform, and the magnetic gradient
          G is too small, the diffusion relaxation can be ignored. The bulk relaxation
          T 2,bulk may not be considered because it takes much longer time than the
          surface relaxation in a tight porous medium. Thus, the T 2 relaxation time
          measured is mainly determined by the surface relaxation. If the pores are
          smaller, the area-volume ratio is larger, T 2 will be shorter. A fluid in large
          pores has higher T 2 value because more nuclei are available to exhibit the
          NMR effect, and the fluid in small pores has lower T 2 value. T 2 relaxation
          time is in inverse proportion to specific surface of samples (Appel, 2004). In
          other words, the pore radius r is proportional to T 2 (Zhao et al., 2015):

                                      T 2 ¼ Cr                       (9.45)
          where C is the conversion constant.
             The above equation can be applied to the system of oil and water that
          covers different areas of the solid A o and A w , respectively:

                                 1      1         A w
                                   ¼         þ r w                   (9.46)
                               T 2;w  T 2;bulk;w  VS w
                                 1       1        A o
                                    ¼        þ r o                   (9.47)
                                T 2;o  T 2;bulk;o  VS o
          where the subscript w and o refer to water and oil, respectively, and S de-
          notes the saturation. It can be understood that if the solid is more water-wet,
          water will cover more of the solid surface. Therefore, the wetting index I w
          may be defined as
                    surface wetted by water   surface wetted by oil
                I w ¼                                                (9.48)
                                    total surface
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