Page 93 - Origin and Prediction of Abnormal Formation Pressures
P. 93

74                         A. GUREVICH, G.V. CHILINGAR, J.O. ROBERTSON AND E AMINZADEH

                             . . . . . . . . . . . . '
                                                  7.                              "
                                           Flow                     Ko     Flow



                             .  .  .  .  .
            Fig.  3-2.  Two extreme  cases  of beds  orientation  with  respect  to fluid flow direction.  (Modified  after Gurevich
            et al.,  1994,  fig.  2,  p.  69.)

            obtain  any  direct  quantitative  evaluations  of  their  manifestation  and  their  influence  on
            fluid pressure  and fluxes in nature.  The list presented above does not include  such rather
            'exotic'  mechanisms  as pressure  increase  due  to  osmotic  processes.  For  such  a process
            to  be  operative,  water  with  higher  salinity  must  be  located  in  a  sand  lens  among  clays
            surrounded  by low-salinity water, and the permeability of the clay must be zero. Clearly,
            such  situations  are rather exotic and do not play any role in regional processes.
               It  is  useful  to  notice  that  the  role  of  each  of  the  mechanisms  listed  above  is
            determined  by  the  rate  at which  the  process  takes  place  and  the  rate at which  pressure
            change is dissipated.

            Role and distribution  of formation permeability

               Permeability  is  a  tensor  value  and  depends  on  space  distribution  of  lithologic
            heterogeneity.  There  are  two  extreme  cases  of distribution  of lithologic  bodies  relative
            to the  direction  of fluid  flow:  alternating  layers  of different  permeability  lie  (1) parallel
            and  (2)  perpendicular  to  the  flow  direction  (Fig.  3-2).  In  the  first  case  the  average
            permeability k~  of the formation for the flow will be:
                           Hi
                         k,i-y                                                  (3-1)
                    -
            where  kli  and  Hi  are  lateral  permeability  and  thickness  of  the  layer  i,  H  is  the  total
            thickness  of the formation.  In the second case, the average permeability k2 will be:
                      ~H'
                 k2  --                                                         (3-2)
                      Hil/k2i
            where  H'  is  the  length  of  the  formation  (in  the  direction  of  flow)  along  which
            permeability  of  rocks  is  being  averaged,  H i'  is  the  thickness  of  layer  i,  and  k2i  is  the
            permeability of this layer along the flow line.
               Gurevich  (1972)  analyzed  the  problem  of  averaging  permeability  of  geological
            formations  for  block  sizes  up  to  a  sedimentary  basin.  It  was  shown  that  regional
            deep  formation  water  flow  velocities,  calculated  on  the  basis  of  regional  permeability
            averaged  as  the  arithmetic  average  from  permeability  values  measured  in  wells  in  oil
            and  gas  fields,  are  in  contradiction  with  hydrogeochemical  zonality  of  groundwater.
            Calculated  (arithmetically  averaged  permeability  values)  velocities  are  at  least  two  or
            three orders  of magnitude higher than it is possible  at the existing geochemical zonality.
            The method of averaging permeability may be the only cause of this discrepancy.
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