Page 269 - Reservoir Formation Damage
P. 269

Two-Phase Formation Damage by Fines Migration  249

             constant  for  deposition  by  pore  throat  plugging.  Civan  (1990,  1996)
             proposed  a dimensionless correlation  to determine  the conditions  favorable
             for  pore  throat  plugging  in  single  phase  fluid  media.  This  equation
             determines  the  critical  ratio  of the pore  throat-to-particle  diameters  below
             which  pore  throat  plugging by jamming  of  particles  occurs. Thus,


                                    <  D./
                k tjjts  = 0 , when D tD p                              (1 1-37)
             For  multi-phase  flow,  this  equation  can  be  modified  as:


                                                                        (11-38)


             where the pore  throat-to-particle diameter  ratio  and the particle Reynolds
             numbers  are  given,  respectively,  by:

                                                                        (11-39)
                Per = A


                                                                        (11-40)



             in  which  the  total  particle  mass  flux  is  given  by:


                               V                                       (11-41)
                      J  J
             and  the  saturation weighted  average  particle  diameter  is  given  by:


                                V                                      (11-42)


                Liu  and Civan (1993,  1995, 1996) have resorted to a simplified  approach
             in  an  adhoc  manner  and  demonstrated  by  comparison  of the  results  with
             experimental  data  that  it  works.  They  assumed  that  the  fraction  of  the
             plugged  pore  throats  is  proportional  to  the  amount of  particles  detained
             behind  the  plugged  pore  throats.  Therefore,  their  expression  for  the
             fraction  of  the  nonplugged pore  throats  can  be  written  as:


                                                                       (11-43)
   264   265   266   267   268   269   270   271   272   273   274