Page 298 - Origin and Prediction of Abnormal Formation Pressures
P. 298

PORE  WATER  COMPACTION   CHEMISTRY   AS  RELATED  TO  OVERPRESSURES   269

                         i       .  .  .  .  .  .  !    9    9   9  '    9  "I   '   '   '   '   .   .   .i   i  --
                   130
             C     120
             0
            ..==                     :   :   :    9 -:   :   :   :   :   :-   ~   .   .~   9  .-
                                     :   :   :  :  :-   -   :    9  :   ::   :   .   :   :  ::
             a                       ~  ~  i           ~ ~i~i~            . . . . . .
                                                       ...-  .i..i-,.-~. ...............................  i..i  .i-!..;.!-
                   110   ...................................   i..:-~.~.!.i  .............................
                       -             i  iiii!          !  i~ii~   ~       ~~i
             C
             fl)          ...........................   i   9  "  ~'"   i  ~  i  ~  ~i   _..*k---,i....'."i   :.  "  -:-"
                                     "  "  ~ . - . ~ . ' . : ; - t ~ ~ ~ . "
                                                                    .  ."*"'i  "  ""..i..~..i..~.'._
             0     100
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                                            .;.
                                                              i.
                                     . ......
             o   O.   90   .....  Na +   "  .~..L.i..;.i.~ ............  ~ ....... ~..."  .~ .... ;..i..i.,.~ ............  ~ .......  ; ..... i .... ;..;..i..~..i.;..-"
            --o        -   _._K   +                                        i i i i ~ -
                                       :
            ._a                       :  ...... :  :  ::   .,  i   i  .  .  ~  ~  i  i  i  ii   :   i   ~  :.  !  ::  ii   -
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                    80   . "--!--...-,.-.-.-Ca  ~+   ~~~~~~   ............ ~-"~,"~  "  .... ~ " ~ ~ ? ~ ? ~  ...............................  ~-~"~.i"i..-   "
                                                                        ~
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                          .,.   Mg   2+   !  i  !  ~ii   ,,i   ~   ~  !  !  ~i   ::  i  i  !~i   -
            .==-
                    70  '  ..............   i  i  iii!  !  ~.  i  !i~!~   ~ ~ ~ -
             O         .  .  .  .  S O 4  2-   .~  9 --:-- -.- -.~ -.~. ! ............ .: ....... .~ .... .. ..~---.-  9 +   9 ~.- :. ! ............  ! ....... ~ ..... .~  9 - -'.: -  9 i  9 - !  9 -!- -.: -:.- - .-
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                    60    -~-  Cl     i  i  iill  i   i   i  i  i!~!  -.k   i   i  i  !  ;iil
                       ..................   "-"':":":"~'~ .............................  ":"~ '"':"-~  ....  -'"'~"'~"~  ..... i .... ~"i"i  i"~*i"-
            o             --..-  TDS   i  i  iili       i  !ii!i      *  ~  ,  ~ "
                                      ~  i  i  iii      i  i  ~  iii   i   ::,,::   i  !  ::  i~
            r~      5 0  "~  ............. ~ ....... ".: ..... i-!---.:--.:---~~  ............ ~ ....... :- .... !-..-.:.--.:---i-.i-.~--~ ............  ,~ ....... i ..... !-..~-..!.i.!-.:-.;..-
                         i  i i iiiiii!  i i i!iiill  i !iiii!ii
                    4 0  --:- ............. :. ....... :- ..... ......i..-:..-..-.!.! ............ ! ....... - .... ~...~...:....i..~..i...: .............. ! ....... ! ..... ! .... !...i..i.!..;.;..,
                              :,   i   i  i  i  :,i~i  i   ~  i  i  i  i  ill  i   :   i  i  i  i  i:i  ,
                        10                1 O0             1000                1 O, 000
                                           Axial  pressure,  psi
            Fig.  10-26.  Relationship   between   the  axial  pressure   and  the  major   ions  expressed   as  a  percentage   of  their
            initial  concentrations   at  50  psi  (0.34  MPa)   in  expelled   pore  water   from   a  kaolinite   clay  (see  Fig.  11-24).
            (Modified   after  Chilingarian   et  al.,  1994,  fig.  5-21,  p.  140.)
            temperature  interval.  These  results  show  that  the  smectite  interlayer  water  represents
            the  only  substantial  available  source  that  can  freshen  pore  fluids  during  the  70 ~  to
            95~  experimental  heating  range,  indicating  that  possibly  little  water  remains  in  the
            smectite  interlayer  regions  by  the  time  the  transformation  of  smectite  to  illite  reaction
            becomes  very  active  at  temperatures  above  212~  (100~   threshold.  Brown's  data  are
            in  general  agreement  with  the  range  of values  reported  by  Colten-Bradley  (1987).  On
            the  other  hand,  Burst's  (1969)  field  observations  indicate  that  the  Gulf  Coast  smectite
            was predominantly  stable until buried  at a depth  of 8000  ft and  a temperature  of  194~
            Rieke  (1972)  attributed  this  observation  to  the  mixed  mineralogy  of  the  argillaceous
            sediments  and  demonstrated  approximate  transitions  based  on  marked  reduction  of
            the  glycolated  17-A  X-ray  diffraction  smectite  peak  from  Gulf  Coast  well  sample
            analysis and autoclave experiments  (Fig.  10-30).  According  to him, the  smectite to illite
            transformation is dependent more on temperature than on pressure (Rieke,  1972, p.  101).
            At  elevated  temperature  and  pressure,  the  smectite  to  illite  conversion  did  not  occur
            when  sodium-  or calcium-smectites were hydrated in water with  various  concentrations
            of  potassium  chloride  and  relatively  short  periods  of  time  up  to  144  h.  Hall  (1993)
            proposed  that  such  smectite-illite  conversion/nonconversion  results,  which  occur  over
            a  wide  range  of temperatures  and  timescales  is  characteristic  of  a  kinetically  hindered
            reaction.  A  kinetically  hindered  reaction  is  one  where  the  cumulative  effect  of  time
            and  temperature  control  the  degree  of  reaction.  Smectite  dehydration  depends  on  the
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