Page 108 - Reservoir Formation Damage
P. 108

Permeability  Relationships  91

             where  n {  and  n 2  are the permeability  reduction  indices,  a  is a  coefficient
             and  K   and  K npg  are  the  permeabilities  at  the  reference  porosities  § PO
             and  § np  of  the  plugging  and  nonplugging  pathways,  respectively.  Eq.
             5-58  represents  the  snow-ball  effect  of  plugging on  permeability, while
             Eq. 5-59 expresses  the power-law  effect  of surface  deposition  on  perme-
             ability.  Eqs.  5-58 and  5-59 have  been  also  verified  by  Gdanski  and
             Shuchart  (1998)  and Bhat  and Kovscek  (1999), respectively,  using  experi-
             mental  data.  Bhat  and  Kovscek  (1999)  have  shown  that  the power-law
             exponent  in Eq. 5-59 can be correlated  as a function of the  coordination
             number  and  the  pore  body  to  throat  aspect  ratio,  applying  the  statistical
             network theory  for  silica  deposition  in  silicaous  diatomite  formation.  Note
             that,  for  n 2 <0  and  £ np/$ npg  «1, Eq. 5-59 simplifies to the expression
             given  by  Gruesbeck  and  Collins  (1982):


                                                                        (5-60)


             where  b = n 2/§ npg.  Eq.  5-60 is  a  result  of  a  truncated  series  approxi-
             mation  of  Eq. 5-59.
                Thus,  substitution of  Eqs. 5-58 and  59  into  Eq.  5-49 results  in  the
             following  expression  for  the  permeability  of  the  porous  media  (Civan,
              1994,  1996):


                                           (l -      )" 2                (5-61)
                K = /,*, oexp(-ae J) + f npK npg  z np/<$> npo
             Cernansky  and  Siroky  (1985)  proposed  an  empirical  relationship  as:




                                         l  E
                                          ~     e x p G l - — M - l     (5-62)
                                       expG-1     1 1     K 0"

             where E  and  G are  some empirical constants. It can  be  shown that  K = K 0
             for  £ = 0.  Civan  (2000)  pointed  out  that,  when E=  1, Eq.  5-62 yields  a
             linear  model  as:



                                                                        (5-63)


             When  E = 0,  Eq.  5-62 yields  a  nonlinear model  as:
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