Page 54 - Origin and Prediction of Abnormal Formation Pressures
P. 54

ORIGIN OF ABNORMAL FORMATION PRESSURES                                 37

            where Crh is horizontal  stress in general.  On assuming  a Poisson ratio,  v, of 0.18  to 0.27
            for consolidated sedimentary rocks, the horizontal compressive stress would range from
            0.22  to  0.37  psi/ft  of  depth.  According  to  Harrison  et  al.  (1954),  for  soft  shales  and
            unconsolidated  sands  found  in  the  Gulf  Coast  of  Texas  and  Louisiana,  which  can  be
            considered to be in a plastic  state of stress,  the horizontal  stresses  are in excess of 0.37
            psi/ft  of depth.  Faulting  can  occur  in  cemented  rocks  at  stresses  that  will  only  cause
            plastic deformation in uncemented rocks.
               The  effective  pressure,  Pe,  may  be  either  increased  or  decreased by  the  presence  of
            vertical  dynamic  flow  and  resulting  fluid  drag  pressure  on  the  grains,  depending  upon
            the  flow direction.  An  example  of this  would  be  quicksand,  a  case  where  intergranular
            loading  has  been  reduced  to  nearly  zero  by  upward  water  seepage  resulting  in  zero
            bearing strength in the skeletal structure.


            Load  transfer
               The overburden (lithostatic) pressure,  Pt, is equal to:

                 Pt  =  Pbg Z                                                  (2-40)
            which  for  all  practical  purposes,  is  the  pressure  exerted  at  any depth  by  the  weight  of
            overlying sediments  and fluids.  The density term in this  equation  is the bulk density of
            fluid-saturated rocks. If Pb is known, the pressure-depth relationships can be established
            in a particular area.
              Hubbert and Rubey (1959, p.  129) stated that within depths of 1 or 2 km, the pressure
            of the water as a function of depth,  D,  can be closely approximated by the equation:

                 Ph  =  pwgD  =  ywD                                           (2-41)
            where  Ph  is  the  hydrostatic  pressure  of  a  column  of water  extending  from  the  surface
            of the  ground  to  a  depth  of  D,  Pw  is  the  density  of the  water,  g  is  the  acceleration  of
            gravity, and  Yw is the specific weight of water.
               Along  the  Gulf  Coast,  the  fluid-pressure  gradient  is  about  0.465  psi  for  each  foot
            of  depth.  This  represents  a  hydrostatic  pressure  gradient  for  brine  having  a  specific
            weight,  yw,  of  67  lb/ft 3.  The  corresponding  shale  matrix  pressure  is  0.535  psi/ft,  if
            one  assumes  a total lithostatic pressure  gradient of  1 psi/ft.  Frederick (1967)  presented
            several  examples  of the  relationship  between  the  bottom  hole  fluid pressure  and  depth
            for areas with abnormal pressures.  Hubbert and Rubey (1959, p.  155) noted a lithostatic
            pressure as high as  1.06 psi/ft occurring in the Khaur Field in Pakistan. Levorsen (1958,
            p. 386) reported that the average gradient of oilfield brines is approximately 0.450 psi/ft.
            Deviations  are  in  part  due  to  the  varying  salt  concentrations  in  the  brines.  Table  2-3
            gives the  specific  gravity and pressure  gradients  of various  fluids  that  might  occur in  a
            sand-shale  sequence.  Fig.  2-8  demonstrates  the  pressure  versus  depth  relationship  for
            various brines.
               AHFPs  can  form  when  a  portion  of  the  effective  stress,  ~e,  normally  assumed  by
            skeletal structure is transferred to the intergranular water.  For example, when increasing
            the  weight  of  the  overlying  sediments  by  continued  burial,  Fz,  at  a  rate  faster  than
            the  intergranular  water  can  escape  from  the  sediment,  the  percentage  of the  lithostatic
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