Page 156 - Origin and Prediction of Abnormal Formation Pressures
P. 156

132                     G.V. CHILINGAR, V.A. SEREBRYAKOV, S.A. KATZ AND J.O. ROBERTSON JR.
                                      Pore  Pressure (pp), MPa

                                    10   20   30       0   10   20   30
                                                            '   qF]  '
                             600                    600
                                                               2Vzz: 1

                                          A)       1200           CB)
                            1200

                         r
                                         \\
                            ~8oo                   1800
                        a


                            2600               \   2600
                                                \
                                                 \
            Fig.  5-3.  Curves  for  estimating  pore  pressure  in  the  formations  of the  Nepsko-Botuobin  anticline  in  East
            Siberia.  (A) Areas with permafrost and average geothermal  gradient  (G2)  of 0.8~   m.  (B) Areas devoid
            of permafrost.  Figures on curves represent geothermal  gradient:  1 =  normal  hydrostatic  pressure gradient;  2
            -- calculated  using the following equation:
                                              O/w
                            Pa  =  gpw(h  --  0.8hi)  --  ~[To.I  -F  (GI  -  G2)h  4-  G2hi]
                                            tip  "t- ~w
            where  tSw is  the  average  density  of  formation  water  at  depth  h;  hi  is  the  thickness  of the  permafrost;  G1
            and  G2  are  geothermal  gradients  respectively  before  and  after  cooling;  T0,1  is  yearly  average  temperature
            of  the  Earth's  surface  prior  to  cooling;  /4p  is  coefficient  of  pore  compressibility  and  flw  is  coefficient  of
            compressibility  of  pore  water;  and  oe,,, is  coefficient  of  thermal  expansion  of  pore  water.  Assumptions  for
            dense  carbonate  rocks:  /4p  ~  flw; tip +  flw  >>  fl~  (/4~ is  compressibility  of  solid  mineral  grains  of rocks);
            C~w >> c~  (c~  is  coefficient  of  thermal  expansion  of  solid  mineral  grains  composing  the  rocks);  Poisson's
            ratio,  v =  0.25;  and  Pi/lSw  ,~  0.75  (,oi is average density  of ice).  (Modified after Dobrynin  and Serebryakov,
            1989,  fig. 51,  p.  108.)

            in  temperature  creates  volume  changes  in  the  rock's  skeletal  structure  and  interstitial
            fluids.  These  processes  operate  only  in  sedimentary  basins  with  aquifer  systems;  they
            do not operate  in infiltration water systems. The  following equation  can be used for the
            estimation  of abnormal  pressure  in  regions  with  uplift plus  erosion,  or  subsidence  plus
            sedimentation (Dobrynin and Serebryakov,  1989):
                 pa  =  Pn  4-  Ap

                      gpw(h   hst)  +   ( I + V )  (tip)gprAh_4_  ~C~w         (5-13)
                                    3(1  -  v)   /~p --~ flw    /~p +/3w  AT
            where  parameters  are  the  same  as  in  Eqs.  5-5,  5-8,  5-9  and  5-10;  Ah  is  the  amplitude
            of  subsidence  or  uplift  and  Pr  is  the  average  density  of new  deposits  after  subsidence
            and  sedimentation.  After the  first  and  second  parts  of Eq.  5-13,  it is necessary to use  a
            minus  sign  in  the  case  of uplift  and  erosion  and  a  plus  sign  in  the  case  of  subsidence
            plus  sedimentation.
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