Page 330 - Origin and Prediction of Abnormal Formation Pressures
P. 330

ABNORMALLY  LOW FORMATION  PRESSURES                                 299

            permafrost,  or  tectonic  uplift  and  erosion.  The  temperature  changed  in  response  to  the
            change in the global Earth's  surface temperature or to the change in depth.
               Such changes may create volumetric changes in (1) rocks,  (2) pore  space, and (3) the
            interstitial  water.  Relative pore  volume  change  dVp/Vp  and  pore  water  volume  change
            dVw/Vw  with respect to a change in temperature can be expressed as follows (Dobrynin,
            1970):


                  Vp   --  j~r d(a  -  p)  +  fis dp  -  as dT                 (11-5)
                 dVw  =  flw dp  -  O~w dT                                     (11-6)
                  Vw
            where  fir, fis, and  fiw, are the coefficients  of compressibility of pore  volume,  solids  and
            water,  respectively;  and  O~s, and  O~w are  the  coefficients  of thermal  expansion  of  solids
            (minerals)  and  water,  respectively.  In  the  case  of  static pore  water  (full  hydrodynamic
            isolation of pores),  a relative change in the volume of pores must be equal to the relative
            change of pore water volume:
                 dVr   dVw
                     =                                                         (11-7)
                  Vr    Vw
            Equating the right-hand sides of Eqs.  11-5 and  11-6, one obtains"
                 flw dp  -  Oew dT  --  fir d(a  -  p)  +  fis dp  -  Ors dT   (11-8)
              Thus,  the change in pore pressure  (dp)  that occurs  during  a change  in the thermody-
            namic conditions of a deposit is equal to:

                           fir           lYw  --  tYs
                 dp  -            da  +           dT                             11-9
                      /~r  -'[- flw  --  fls   fir  -[-  flw  --  fls
                                                                       1
                                                                 2
               The  average  normal  stress  (a)  for  horizontal  layers  is  a  --  5ax  +  5az,  where  ax  is
            the horizontal  component  of  stress  (and  ax  --  ay),  and  az  is  the  vertical  component  of
            stress. Using the mean lateral compression:
                             l)
                           ~ a
                 Crx  --  Oy  =  1_  v   z                                    (11-10)
            The total overburden  stress is equal to"

                               a z                                             (11-11)
                 a   3  1-v
                     -
                   -
            where  v is Poisson's ratio.
               Differentiating Eq.  11-11  one obtains:
                       1  [l+V]d,                                              (11-12)
                 da--~    1-v
            where  da z  is  the  change  in  the  vertical  component  of  stress  during  sedimentation  or
            erosion. Expressing da z in terms of change in sedimentary overburden,  one obtains:

                       1  [l+VlgprAh                                           (11-13)
                 da-~     1-v
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