Page 50 - Origin and Prediction of Abnormal Formation Pressures
P. 50

ORIGIN  OF ABNORMAL FORMATION PRESSURES                                3 3

            where  crl  is  the  total  major  stress,  ~r2  is  the  total  intermediate  stress  and  or3  is  the  total
            minor  stress.
               According  to Lo  (1969),  the physical justification  for Eq.  2-30  lies  in  the  fact that un-
            der  ambient  stress,  the  induced  pore  pressure  corresponds  almost  exactly  to  the  applied
            pressure,  because  the  compressibility  of the pore  water  and  argillaceous  sediment  grains
            are  much  lower  than  that  of the  sediment  structure.  Most  of the  pore-pressure  equations
            presented  in literature  give  almost  identical  results  providing  they  are properly  used.  For
            further  detailed  discussion  see Rieke  and  Chilingarian  (1974).

            Spring models of compaction

               The  concept  of the  shale-compaction  process  can  be  best  explained  by  a  mechanical
            model  which  is  composed  of  a  perforated,  round  metal  plate  and  the  enclosing  cylinder
            which  contains  a  metal  spring  and  water  (Fig.  2-5).  In  this  analogy,  the  spring  represents
            the  compressible  clay  particles,  the  water  represents  the  fluid  in  the  pore  space,  and  the
            size  of the perforations  in the  metal  plate  determines  the permeability.
               Using  this  model,  well-saturated  clay  can  be  treated  mathematically,  as  a  two-phase
            continuum.  The  hydrated  clay  is  envisioned  as  clean  clay  plates  in  mechanical  contact


                            A               B               C               D
                      Overburden  Pressure   Overburden  Pressure
                          0  psig         25 psig      Overburden  Pressure
                             =                9           25 psig
                                                                       Overburden  Pressure
                                                                          25  psig
                                 Perforated  plate
                                  /  /
                                 /  t.t
            Manometer










                        or'=  0psig    ~'=   0psig     or'=  3psig     ~'=  25psig
                        ~w =  0  psig   crw =  25 psig   ~  =  22  psig   crw =  0  psig
                        )~  =infinity  ~L  =   I       )~   -   0.875  X   =   0
            Fig.  2-5. Compaction  analogy using  a spring  and perforated plate,  o -t is the effective  (intergranular)  stress,
            ~w is the pore-water stress and X is the ratio of the pore-water stress to the overburden stress on the system
            (c~ t and Crw are in psig).  (Case A) Initial conditions;  tightly fitted, frictionless  metal plate seals the water in
            the cylinder. There is no  overburden  load on the  system and perforations of plate  are sealed.  (Case  B)  A
            25-psig  load is imposed on the model.  This  load is  entirely carried by the water. Perforations in the plate
            are  sealed.  (Case  C) The  fluid is  allowed to  flow out through the perforations.  The  plate  descends  as  the
            fluid escapes.  The  spring carries  a portion of the load.  (Case D) The spring  now carries  the entire  25 psig
            load. The system is in equilibrium  and there is no water outflow. (Modified after Taylor, 1948; in Rieke and
            Chilingarian,  1974, fig. 49, p. 90.)
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