Page 155 - Formation Damage during Improved Oil Recovery Fundamentals and Applications
P. 155

Formation Damage by Fines Migration: Mathematical and Laboratory Modeling, Field Cases  133


              2
              c X w 1T;TÞ
               ð
                        0                           1
               8
                            Λ    p
               >                  ffiffiffiffi p ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi
               >
               >                  X2
                        @  p           ð            A
               >                        12αÞX1αX w    ; T,X mI 2X w
                S aI =φ exp 2 ffiffiffiffiffiffi
               >
                             X w
               >
               >
               >
               >
               >
               >         0         1
               >
                   1          q
               >
               >
               >
               >                ffiffiffiffi;γ
               >       S cr  @  p  A
               >  12αÞφ            I
                 ð         2πr e X
               >
               >
               >
               >
               >
               >
                            0                            1
               >
                                 Λ
               >
               >
               >                     p ffiffiffiffi p ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi
               >
               >                      X2
                            @   p           ð            A
               >   1S aI =φ exp 2 ffiffiffiffiffiffi    12αÞX1αX w     ; X mI 2X w ,T,T mI
               >
               >                 X w
               >
               >
               >
               >
               >         0         1    0      0          11
               >
                   1         q         1            q
               >
               >
               >
               >               ffiffiffiffi;γ  1              ffiffiffiffi;γ
               >       S cr  @  p  I  A  @  S aI 2S cr  @  p  I  AA
               >  12αÞφ                φ
                ð         2πr e X                2πr e X
               >
               >
               >
               >
               >
               >
                             0                           1
               >
               >
               >                 Λ    p
               >                       ffiffiffiffi p ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi
               >
               >                       X2
                             @  p                        A
               >                            ð 12αÞX1αX w   ; T mI ,T,X mJ 2X w
                          exp 2 ffiffiffiffiffiffi
               >
                                 X w
               >
               <
             5         2  0          1    0          13    0      0          11;
               >
               >   1           q               q         1             q
               >
               >               p ffiffiffiffi;γ        p ffiffiffiffi;γ  1             p ffiffiffiffi;γ
               >       4 S cr  @     A 2S cr  @      A5    @  S aI 2S cr  @  AA
               >  12αÞφ             I               J    φ                  I
                 ð          2πr e X         2πr e X                 2πr e X
               >
               >
               >
               >
               >
               >          0                            1
               >
                               Λ
               >
               >                   p
               >                    ffiffiffiffi p ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi
               >
               >                    X2
                          @  p           ð             A
               >       exp 2 ffiffiffiffiffiffi       12αÞX1αX w    ; X mJ 2X w ,T,X crI 2X w
               >
               >               X w
               >
               >
               >
               >
               >             2      0          13    0      0          11
               >
                         1               q          1            q
               >
               >
               >
               >                           ffiffiffiffi;γ  1               ffiffiffiffi;γ
               >             4 S aI 2S cr  @  p  J  A5  @ S aI 2S cr  @  p  I  AA
               >       12αÞφ                       φ
               >       ð              2πr e X                 2πr e X
               >
               >
               >
               >
               >
                        0                           1
               >
               >
               >            Λ    p
               >                  ffiffiffiffi p ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi
               >
               >        @  p      X2   ð 12αÞX1αX w  A ; X crI 2X w ,T,T crI
                     exp 2 ffiffiffiffiffiffi
               >
               >
               >             X w
               >
               >
               >
               >
                                   2      0          13
               >
               >
               >
               >               1               q
               >                                 ffiffiffiffi;γ
               >                                        ;
               >                   4 S aI 2S cr  @  p  J  A5  T.T crI
               >             12αÞφ
               :             ð              2πr e X
                                                                        (3.139)
              where,
                           X mJ 2 X w    X mI 2 X w     X crI 2 X w
                      T mJ 5       ; T mI 5      ; T crI 5      :       (3.140)
                             1 2 α         1 2 α          1 2 α
                 Eq. (3.139) is the boundary condition for the solution of Eq. (3.132)
              in zones 4 9in Fig. 3.21B. Applying the method of characteristics yields
              explicit formulae for the suspended concentration in zones 4 to 9 (rows
              11 to 16 in Table 3.8).
   150   151   152   153   154   155   156   157   158   159   160