Page 92 - Origin and Prediction of Abnormal Formation Pressures
P. 92

ORIGIN  OF FORMATION FLUID PRESSURE  DISTRIBUTIONS                    73

               (b)  Piezo-convection  effect.  In  the  convective  rise  of  gas,  changing  places  with
               the  liquid  that  it  displaces,  the  gas  enters  a  region  of  lower  pressure,  whereas  the
               liquid  enters  a  region  of  higher  pressure.  But  because  of  the  great  difference  in
               their  compressibilities  (and  the  lower  the  pressure,  the  greater  this  difference),  the
               expansion  of gas  must  be  much  greater  than  the  compression  of the  liquid  that  has
               arrived at the  former  site of gas.  If the  volume  in  fluid-saturated  rocks  in which  this
               convective  redistribution  of  fluids  takes  place  is  poorly  permeable  or,  especially,  if
               it  is  surrounded  by  poorly  permeable  rocks,  the  outflow  of fluid  compensating  this
               difference  in  new  volumes  will proceed  very  slowly.  Therefore,  a  significant  (local)
              increase  in  pressure  will  arise,  by  means  of which,  through  additional  compression
               of both  liquid  and  gas,  the  greater  expansion  of the  gas  will  be  compensated,  thus
              preserving the overall balance of volume. This effect will be the greatest in vertically
              fractured zones in poorly permeable rock formations.
            (3) Effects of temperature change:
              (a) Thermoelastic  effect.  Inasmuch  as the coefficient of thermal expansion is greater
              for fluids than for rock and,  therefore,  for the pore  space,  an increase  in temperature
              will increase the pressure,  and a drop in temperature will lower the pressure.
              (b)  Changes  in  the  state  of  aggregation,  i.e.,  ice/water  and  water/vapor  phase
              transitions  as  the  temperature  passes  through  a  critical  point.  Also  included  here  is
              the  transition  of  bound  water  to  free  water  as  the  temperature  is  raised  (with  an
              increase in pressure),  as well as the reverse transition of free water into bound  water
              when temperature is lowered (with a decrease in pressure).
              (c)  Precipitation  of  salts  from  saturated  solutions,  when  the  temperature  is  lowered
              and the salt solubility is reduced,  generally leads to a decrease in pore volume and an
              increase in pressure.  Dissolution of salts, when temperature is raised, usually leads to
              an increase in the pore volume and a drop in pressure.
              (d) Generation of oil and gas by thermocatalytic transformation of organic matter and
              the  decomposition  of carbonates  to  form  carbon  dioxide  (in  quantities  greater  than
              the quantities that can be dissolved in the pore water),  accompanied by the formation
              of new fluid and an increase in pressure.
               (e)  Dehydration  of  minerals.  Transformation  of  montmorillonite  to  illite,  gypsum
              to  anhydrite,  and  analogous  transformations  of  other  minerals  lead  to  increases  in
              pressure.
            (4)  Chemical  transformations  of  substances  that  are  not  initiated  by  temperature
            increase,  such  as  radiochemical  decomposition  of  water  and  hydrocarbon  molecules,
            thermochemical  decomposition  of  hydrocarbon  molecules,  synthesis  of  molecules  of
            resins  and  asphaltenes,  and  dolomitization  of  limestone.  These  phenomena  have  not
            been yet evaluated rigorously in terms of the overall change in the volume of the system
            and its impact on pressure.

               This, in brief, is the list of basic thermodynamic phenomena (physical, physicochem-
            ical,  and  chemical  in  character)  leading  to  changes  in  the  specific  amount  and  degree
            of  compression  of  a  fluid  in  the  intergranular  space  of rocks.  It  must  be  emphasized
            that  even  though  the  nature  of  these  mechanisms  and  individual  processes  and  their
            qualitative  patterns  are  rather  clear  in  most  cases,  it may  still be  extremely  difficult  to
   87   88   89   90   91   92   93   94   95   96   97