Page 131 - Geochemical Remote Sensing of The Sub-Surface
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108                                                           S.M. Hamilton

           negative  redox  anisotropy  in  groundwater-saturated  basal  overburden   over
           mineralisation  relative  to  the  surrounding  overburden  over  country  rock.  Whilst
           electronic  current  continues,  there  must  be  continual  outward  dissipation  of  negative
           charge  into  surrounding  overburden;  otherwise  the  build-up  of  reducing  conditions
           around  the  top  of  the  conductor  would  eliminate  the  voltage  differential  and  current
           would  cease.  Once  solid-phase  oxidising  agents  are  consumed,  this  dissipation  of
           negative charge must take place by the outward migration of reduced ions away from, or
           the  inward  migration  of  oxidised  ionic  species  toward,  the  cathode.  This  process  is
           necessarily  coupled  with  oxidation-reduction  reactions,  occurring  between  the  top
           surface  of the  conductor  and  the  water  table,  that  involve  both  reduced  and  oxidised
           species.  The dissipation of negative charge away from the conductor is accomplished as
           the oxidation states of reduced species change during this process, resulting in dissolved,
           gaseous  or  precipitated  products  that  have  a  higher  redox  potential  than  the  reduced
           reactants.
              Figure 3-9 provides a hypothetical example of the possible outcome of this process in
           young,  exotic  sediments.  Figure  3-9A  depicts  a  fine-grained  glacial  material,  shortly
           after  deposition,  in  which  a  background  redox  differential  of  150  mV  exists  between
           groundwater  at  the  water  table  and  in  basal  overburden  units.  An  electronically-
           conductive,  steeply-dipping  mineral  deposit  occurs  in  bedrock.  More  reducing
           conditions  immediately  above  the  conductor  result  in  a  redox  differential  of  300  mV
           between  the  top  of mineralisation  and  the  water  table.  Spontaneous  potential  contrasts
           exceeding  150 mV between conductive mineralisation and adjacent rock have often been
           reported (e.g., Pflug et al.,  1996; Bolviken and Logn,  1975).
              At the time of overburden deposition, a very strong vertical redox gradient exists just
           above  the  bedrock  conductor  along which  ions  have  a  tendency  to  move.  The  outward
           movement  of  reduced  ions  such  as  HS,  Fe 2+ or  $2032- results  in  the  migration  of  a
           reduced  front  away  from  mineralisation.  At  the  front,  reduced  ions  come  into  contact
           with oxidising agents and redox reactions take place, thereby dissipating negative charge
           away from the conductor.  Once the front reaches the water table,  a reduced  column will
           have developed in the groundwater-saturated overburden above mineralisation.
              If  the  capacity  for  electrical  current  in  the  conductor  is  high,  the  production  of
           reduced  species  might exceed  the capacity of the  unsaturated  zone  above  the  column to
           provide  oxygen  across  the  water-table  phase  boundary.  In  this  case,  the  column  would
           probably widen out. As it widens, the surface area exposed to oxidising agents along the
           entire  reducing  front  increases.  Once  the  column  diameter  is  sufficiently  large,  the
           capability  of  the  water-table  phase  boundary  and  surrounding  overburden  to  provide
           oxidising agents  equals  that of the  conductor to provide negative charge.  The  supply of
           oxidising  and  reducing  agents  is  therefore  balanced  and  a  steady-state  kinetic
           equilibrium  is  established  between  the  two processes  within  the  cell.  The  equipotential
           lines  around  the  column  above  the  conductor  cease  to  move  outward  and  their
           previously-horizontal  configuration  becomes  nearly  vertical  in  the  vicinity  of  the
           reduced column. The end result is a permanent Eh anisotropy in overburden between the
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