Page 166 - Reservoir Formation Damage
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148   Reservoir Formation Damage

               Electrostatic  Double-Layer  Force.  These  forces  are  created  due  to  the
               ionic  conditions  measured  by  pH  and  ionic  strength.  When  the  particle
               and  grain  surfaces  carry  the  electrostatic  charges  of  the  same  sign,  they
               repel  each  other.  The  repulsive  force  is  expressed  by  (Ives,  1985):



                                                                           (8-10)
                          +  Qxp[-kd(s-2)]

               where  s  is  the  dimensionless  separation  distance  expressed  as  the  ratio
               of  the  radial  separation  distance  divided  by  the  particle  radius  (d/2),  k  is
               the  Debye reciprocal  double-layer  thickness, and d is the particle diameter.
               When   the  ionic  strength  is  higher,  then  the  double-layer  thickness  is
               smaller,  and  hence  k  is  larger.

               Born  Repulsion  Force.  This  force  is  generated  as  a result  of  the  over-
               lapping  of  the  election  clouds  (Wojtanowicz  et  al.,  1987, 1988).

                               Rate  Equations   for  Participate
                                Processes   in  Porous  Matrix
                  Ohen  and  Civan  (1993)  classified  the  indigenous  particles  that  are
               exposed  to  solution  in  the  pore  space  in  two  groups:  lump  of  total
               expansive  (swelling,  that  is,  total  authigenic  clay  that  is  smectitic)  and
               lump  of  total  nonexpansive (nonswelling) particles,  because  of  the  differ-
               ence  of  their  rates  of  mobilization  and  sweepage  from  the  pore  surface.
               They  considered  that the  particles  in  the  flowing  suspension are  made of
               a  combination  of  the  indigenous  particles  of  porous  media  entrained  by
               the flowing  suspension and the external  particles  introduced to the porous
               media  via  the  injection  of  external  fluids.  They  considered  that  the
               particles  of  the  flowing  suspension  can  be  redeposited  and  reentrained
               during  their migration  through  porous  media  and the rates of  mobilization
               of  the  redeposited  particles  should obey  a different  order  of magnitude than
               the indigenous particles  of the porous  media.  Further,  they assumed that the
               deposition  of  the  suspended  particles  over  the  indigenous  particles  of  the
               porous  media  blocks  the  indigenous  particles  and  limits  their  contact  and
               interaction  with  the  flowing  suspension  in  the  pore  space.  They  considered
               that  the  swelling  clays  of  the  porous  media  can  absorb  water  and  swell  to
               reduce  the  porosity  until  they  are  mobilized  by  the  flowing  suspension.
                  The  rate  at  which  the  various  paniculate  processes  occur  in  porous
               media  can be expressed  by  empirical  equations.  These  equations  can  also
               be considered  as the particulate material  balance  equations  for the porous
               matrix.  Here  they  are  written  as  volume  balance  of  particles.
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