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Spontaneous potentials and electrochemical cells                      105


           gradient  that  exists  in the  Earth's  crust.  The  conductor  provides  a  less  resistive  route  to
           upward  flow  of negative  current  from  depth  and  concentrates  the  background  current,
           thereby  short-circuiting  the  redox  field.  The  conductor  and  redox  field  combined
           represent  the  voltaic  cell:  without  the  redox  field,  there  would  be  no  reactants;  and
           without the conductor there would be no focusing of current and hence no cell.
              The  consumption  of oxidising  agents  around  the  upper part  of the  conductor  results
           in  more  reducing  conditions  immediately  around  the  top  of  the  conductor  than  in
           adjacent  areas  (Hamilton,  1998).  Likewise,  locally-anomalous  oxidised  conditions
           develop  around  the  bottom  of  the  conductor  because  of  the  consumption  of  reducing
           agents.  However,  conditions  can never become  as reducing at the top of the conductor  as
           they  are  at  the  lower  end  or  all  current  would  cease.  The  result  of  the  process  is  to
           modify  the  shape  of the  redox  field  around  the  conductor  (Fig.  3-7).  This  also  modifies
           the lines of current flux since,  in isotropic  media,  current moves perpendicular to lines of
           equal potential.
              The specific  redox half-reactions  that result in current flow through  the conductor  are
           of  less  importance  than  their  aggregate  effect  on  voltage.  The  stability  field  of  water
           restricts  the  overall  voltage  of the  cell  to  less  than  1500  mV.  Redox  reactions  involving
           the reduction  or oxidation  of water,  such  as occur  in most electrolytic  cells,  are  unlikely
           to  be  part  of  the  SP  charge-transfer  mechanism  despite  contrary  statements  by  some
           authors (Bolviken and Logn,  1975;  Sivenas and Beales,  1982;  Clark,  1997).
              Electrochemical  cells  after  the  model  of  Sato  and  Mooney  (1960)  develop  due  to
           zones  of  anomalously-high  electrical  conductivity  in  Earth  materials  in  what  would
           otherwise be  a roughly uniform  vertical redox gradient.  The  issue of the conductor being
           electronically  conductive  is,  perhaps,  a  red  herring.  A  zone  of  fault  gouge  made  up  of
           water-saturated  rock  flour  and  phylosilicates  could  conceivably  have  a  very  high
           electrolytic  electrical  conductivity,  especially  relative  to  surrounding  poorly-fractured
           rock.  This  should  also  develop  a  significant  electrical  current  within  it,  provided  an
           upward-increasing redox gradient also exists.
              Two  hidden  assumptions  implicit  in  the  model  of Sato  and  Mooney  (1960)  are:  (1)
           that  the  conductor  consists  of  a  single  phase,  such  as  graphite  or  pyrite;  and  (2)  that
           oxidation  of  the  conductor  would  result  in  its  conversion  to  a  non-conductive  phase.
           Thornber  (1975a,  1975b)  presents  a  reactive  conductor  model  in  which  the  conductor
           itself  is  the  reducing  agent,  which  is  in  apparent  contrast  to  the  model  of  Sato  and
           Mooney.  However,  the  reactive  conductor  model  is  based  on  the  presence  of  one
           oxidised phase  and at least one reduced phase  relative to the  first phase,  all of which  are
           electronically  conductive.  Such  scenarios  have  been  noted  in  terrain  with  deep
           weathering  profiles  due  to  the  phase  conversion  of reduced  sulphide  minerals  to  more
           oxidised forms.
              A  sulphide  body  containing  pyrrhotite  in  its  lower part and pyrite  in  its upper part  is
           an example  of such  a cell  (Fig.  3-8).  Pyrrhotite  at the boundary  between  the  two  phases
           oxidises to form pyrite, which remains electronically conductive.  Electrons  liberated  into
           the  sulphide  mineralisation  move  up  toward  the  more  oxidising  environment  and  allow
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