Page 136 - Formation Damage during Improved Oil Recovery Fundamentals and Applications
P. 136

116                                                 Thomas Russell et al.


             Solving Eq. (3.105) by separation of variables, accounting for initial
          condition (Eq. (3.99)), yields C(X,T) 5 0 ahead of the salinity front.
             To find a solution between the suspended particle and the salinity front,
          zone (αT , X , T), it is necessary to calculate the boundary condition for
          suspended particle concentration behind the front X 5 T. Consider the mass
          balance condition on the salinity front (Bedrikovetsky, 1993; Lake, 2010):

                                ½ C 1 S s 1 S a ŠD 5 α C ½Š;         (3.106)

          where D is the shock front velocity, and jump of the quantity A is the
                                                                      1
          difference between A-values ahead and behind the front: [A] 5 A -A 2
          (Polyanin and Zaitsev, 2011; Polyanin and Manzhirov, 2007). As it follows
          from the kinetics Eq. (3.95), the strained concentration is continuous
          across the shock. The values of the attached concentration ahead and
          behind the shock follow from the solution (Eq. (3.102)), and the value of
          the suspended concentration ahead of the shock follows from the solution
          to Eq. (3.103) for zone 0:


                                   1
                                                 2
                           1

                         C 5 0; S a 5 S cr γ ; S a 5 S cr γ ;        (3.107)
                                            I            J
          and as the shock is being evaluated across the line X 5 T, the shock veloc-
          ity equals one.
             Substituting Eq. (3.107) into Eq. (3.106) yields the suspended concen-
          tration behind the salinity front:
                                            1
                                    C 5          :                   (3.108)
                                         ð 1 2 αÞφ
             Solving Eq. (3.105) by separation of variables, accounting for the
          boundary condition for suspended particle concentration behind the front
          X 5 T, yields:

                                     1               T 2 X
                       CX; TÞ 5          exp 2αΛ              :      (3.109)
                         ð
                                 ð 1 2 αÞφ           1 2 α
             Using the method of characteristics for Eq. (3.103) along with the
          boundary condition (Eq. (3.100)) yields a zero suspended concentration
          C(X,T) 5 0 behind the suspended particle front X 5 αT, zone 2.
             The strained concentration is obtained from Eq. (3.95) by integration
          of the suspended concentration in time. Table 3.5 presents a summary of
          the solutions for salt transport, and attached, suspended, and strained con-
          centrations in the different zones.
   131   132   133   134   135   136   137   138   139   140   141