Page 118 - The Geological Interpretation of Well Logs
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-  THE  GEOLOGICAL  INTERPRETATION  OF  WELL  LOGS  -




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        Figure  8.27  A  sonic  log  re-played  on  a  lime  scale  furnished  with  a  lithology  and  stratigraphy,  gives  an  accurate  visual  geology  to
        the  seismic  section.
        (top  horizontal  scale)  then  becomes  compatible  with  the   the  average  velocities  between  check  shots  correspond
        seismic  section.  A  normal  time-depth  curve  is  taken  from   to  the  average  velocities  on  the  sonic  log  (Goetz  ef  ai.,
        zero  time  and  zero  depth  (i.e.  corrected  from  well  KB  to   1979),  With  the  achieved  precision,  the  sonic  log  may
        a  surface  datum  which  is  mean  sea  level  offshore)  to  the   now  be  replotied  by  the  computer  on  a  linear  time  scale
        weil  TD.  From  this  can  be  read  the  average  time  to  any   similar  to  that  of  a  seismic  section  (say  1Ocm  =  |  second)
        particular  depth  or  stratigraphic  horizon,  and  this  value   rather  than  a  linear  depth  scale  as  in  a  well  (Figure  8.27).
        can  then  be  used  to  convert  seismic  time  maps  (isochron   A  geological  and  stratigraphic  representation  on  a  time-
        maps)  to  depth  maps  (isobath  maps).  But  it  should  be   scale  log  is  a  powerful  tool  for  both  geophysicist  and
        remembered  that  time-depth  curves  are  in  one-way  time   geologist.  The  seismic  section  takes  on  a  direct  geological
        and  seismic  sections  and  isochron  maps  are  in  fvo-way   significance  (Figure  8.27).
        time  (the  time  it  takes  for  a  seismic  signal  to  go  from  the
        surface  to  the  reflector  and  back).          Synthetic  seismic  logs
          In  practice,  when  a  well  is  completed  a  series  of  ‘check   A  synthetic  seismic  log  is  a  presentation  of  the  data
        shots’  is  run  to  calibrate  the  sonic  log.  That  is,  a  geophone   contained  in  a  sonic  log  in  the  form  of  a  seismic  trace.
        is  lowered  into  the  well  and  a  shot  is  fired  at  the  surface.   In  a  computer-derived  calculation,  the  high  frequency
        The  time  taken  by  the  sound  pulse  from  the  surface  to   data  of  the  sonic  log  is  replayed  at  the  low  frequency  of
        reach  the  geophone  is  recorded.  The  precise  depth  of  the   seismic  data.
        geophone  is  known  and  therefore  also  the  precise  time  to   A  seismic  section  is  the  result  of  acoustic  reflections
        this  depth.  The  shots  are  made  throughout  the  boretiole   from  subsurface  strata.  The  reflections  depend  on  the  con-
        either  with  the  geophone  at  strategic  stratigraphic  and   trasts  of  the  acoustic  impedances  (i.e.  velocity  X  density)
        seismic  levels  (just  above  a  probable  reflector)  or,  more   of  the  adjacent  layers,  that  is  the  reflection  coefficient  (R):
        commonly  nowadays  at  regular  close  intervals  such  as
                                                            Re  acoustic  impedance  below  acoustic  impedance  above
        every  25m  or  50m.  A  time-depth  curve  can  be  made  from
                                                               acoustic  impedance  above+  acoustic  impedance  below
        the  check  shots  which  is  independent  of  the  sonic-derived
        time-depth  curve.  Alternatively,  the  check-shot  depths
                                                                                  ~
                                                                                    DV,
        may  be  used  by  relating  them  to  the  sonic  log,  the  latter   DV,
                                                                         1.€.
        then  being  squeezed  or  stretched  from  shot  to  shot  so  that   DY,  +  DY,
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