Page 21 - Origin and Prediction of Abnormal Formation Pressures
P. 21

4                    E.C. DONALDSON, G.V. CHILINGAR, J.O. ROBERTSON JR. AND V. SEREBRYAKOV

            psi/ft).  In the  geopressured  reservoirs  of the  Gulf Coast  region  of the  United  States,  at
            a depths  greater than  3000  m,  the pressure  gradient increases  to  about  20.3  kPa/m  (0.9
            psi/ft).  Hence,  fluids  in  the  geopressured  zones  can  exhibit  pressures  greater  than  68
            MPa  (about  10,000  psi).  The formation  with normal  pressure  gradient  and  the geopres-
            sured zone  above can coexist only if they are separated by barriers that are impermeable
            to the vertical movement of fluids  over millions  of years of geologic time.  The pressure
            seals (caprocks)  above the geopressured  zones are impermeable to the flow of fluids.

            Undercompaction

               Undercompaction  of the  sediments  can  occur  during  rapid  sedimentation  and burial
            of  sediments  containing  a  large  quantity  of  clay  minerals  (Rubey  and  Hubbert,  1959;
            Wilson  et  al.,  1977).  The  complete  expulsion  of  water  does  not  occur,  leaving  the
            sediments as a loosely bound  system of swollen clay particles with interlayer water.
               Where  rapid  deposition  involves  large  quantities  of  clays,  the  sand  bodies  can  be
            surrounded  by  clays,  and  if the  loading  rate  of sediments  is high,  the  permeability  will
            decrease  rapidly.  Consequently,  the  pore  fluids  are  prevented  from  escaping  vertically
            through  the  overlying  argillaceous  sediments.  Support  of  the  overburden  load  is  then
            transferred  to  the  interstitial  fluids  and  the  formation  becomes  abnormally  pressured
            because  the  fluids  are  subjected  to  the  load  of  the  newly  deposited  sediments.  Thus
            fluids  support a greater portion  of the total overburden  load (see Eq.  1-3).
               If  the  rate  of  migration  of  water  from  the  formation  undergoing  sedimentation  is
            equal  to  the  rate  of  sedimentation,  the  excess  fluid  pressure  created  by  the  increasing
            loading  will  be  dissipated  and  hydrostatic  pressure  will  be  maintained  at  all  depths  as
            the compaction  of sediments takes place (Johnson  and Bredeson,  1971).

            Tectonic compression

               Lateral  compression  can  occur  in  orogenic  belts  resulting  in  development  of abnor-
            mally  high  pore  pressures.  Cretaceous  mudstones  of  northern  Wyoming  (USA)  have
            been deformed  by lateral compression,  which has decreased the formation  porosity with
            consequent  fluid  expulsion  through  permeable  beds  or  increase  of  formation  pressure
            within  the  sealed  zones  (Rubey  and  Hubbert,  1959).  Fluid  pressure  almost  equal  to
            the  overburden  pressure  was  encountered  during  the  initial  drilling  of  the  Ventura
            Field  (California).  The  presence  of these  faulted  and  folded  zones  suggests  that lateral
            tectonic  stresses  are  responsible  for  some  of  the  surpressures  that  were  encountered
            (Watts,  1948).  Anderson  (1927)  reported  that abnormally high formation pressures  were
            encountered  on  the  Potwar  Plateau  of  West  Pakistan  just  south  of  a  folding  zone  in
            the foothills  of the Himalaya Mountains;  high  fluid  pressures  were  also  associated with
            folding  in the Khaur Field of West Pakistan  (Keep and Ward,  1934).
              As  a  result  of  the  compressive  forces,  water  from  shales  can  be  squeezed  into  the
            associated  reservoir  rocks  (sandstones  or  carbonates),  giving  rise  to  overpressures  (see
            Chapter 8).
              A  cubic  element  in  the  subsurface  has  nine  stress  components  acting  on  it:  three
            principal,  normal  stresses,  cri, acting  on  the  planes  normal  to  the  major  axes  and  six
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