Page 240 - Reservoir Formation Damage
P. 240

220    Reservoir Formation Damage

                Applications   of  the  Ceriiansky  and  Siroky  Model

                  The  objectives  of  the  experimental  studies  were  threefold:

                  1.  Determine  an  empirical  relationship  between  permeability  and
                     porosity  in  the  form  of  Eq.  10-92.
                  2.  Determine  the  values  of  the  deposition  and  entrainment  rate con-
                     stants,  k p  and  k' e.
                  3.  Study the  effects  of  the  length  of  porous  media  and  the  rate  and  con-
                     centration  of the particle  suspension  injected into the porous  media.

                  The  pressure  difference  across  the  porous  media  and  the  particle
                concentration  of  the  effluent  were  measured  as  functions  of  time during
                the  injection  of  a  suspension  of  finely  ground  limestone  particles  at  a
                given  concentration  and  rate.
                  The porous  material  was  prepared  by  using nonwoven felt  of filaments
                of polypropylene.  The porous  material  samples  of  4 cm diameter and 0.5,
                1.0,  1.5, and  2.0  cm  lengths  were  used.  The  particle  suspension  was
                                                                3
                prepared  using finely  ground  limestone  of  2,825 kg/m  density  in  water.
                The  porosity  was  determined  by  the  weighting  method.  The  discrete
                times  at  which  measurements  are  taken  are  denoted  by  the  subscript
                i = 2,3,...,N  and  the  initial  time  is  denoted  by  /  =  1. The  permeability
                was  determined  by  Darcy's  equation  by  neglecting  the  effect  of  gravity
                for  short  samples:

                   KI  = wjiL/A/?,.  : i = 2,3,..., TV                   (10-170)

                  The  volume  of  particles  deposited  per  unit  volume of porous  media  was
                calculated,  by  integrating Eq.  10-84  and  applying the  mean value theorem:



                    <te]  = I  f fk  dx = K-^>                           (10-171)
                    dt)     Ljdtdt         L
                                            L
                              o
                from  which

                            t
                            f
                  e = e  +- fa   -a   }dt Ul                             (10-172)
                  C
                       °  T  \ V  '"  OUt)
                            O
                where  £ 0 =0  for an initially particle-free  porous  material.  Eq.  10-172 is
                evaluated  numerically by  applying  the  trapezoidal  rule  of  integration  as,
                for  a  constant  injection  suspension  particle  concentration:
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