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Zhigniew KoczorowskiA
                                   32
                                   the  metal  and  the  potential  across  the  emerging  double  layer  of  the  bulk
                                   electrode)  transferred  into  an  emersed  state  evidently  remain  intact. 81–84
                                   The  1: 1  correlation  between  the  Volta  and  emersion  potentials  i.e.,= the
                                   potential  supplied  prior  to  emersion)  presents  a  strong  argument  in  favor
                                   of  the  above  conclusion.= However,  the  removal  of  the  double  layer
                                   becomes  less  perfect  with  decreasing  ionic  strength  of  the  electrolyte
                                   (< 0.1 M) because of the increasing extension of the diffuse part of the
                                   double  layer.= A  1  : 1  correlation  of the  Volta potential  with  the  emersion
                                   potential has been found also for electrodes coated with exchange polymer
                                   membranes. 85–86
                                       The emersed electrode, in principle,  may be treated as the experimen-
                                   tal  realization  of  a  single  electrode.= However,  it  is  doubtful  whether  its
                                   liquid layer has the same bulk properties.= This is probably=the main reason
                                                           o
                                   for  the  different  results  of  E H (abs)  found  for  emersed  electrodes,  e.g.,=
                                                       87
                                   –4.85  V.83 Samec  et  al.   have  found  that  emersion  of  electrodes  in  a
                                   nitrogen  atmosphere  decreases  the  Volta potential  and  therefore  the  abso-
                                   lute electrode potential by ca.=0.32 V relative to the value in solution.=They
                                   have  attributed  this  mainly  to  the  reorientation  of  the  water  molecules  at
                                   the free  surface.=
                                                                         88
                                       The non situ experiment pioneered by Sass  uses a preparation of an
                                   electrode in an ultrahigh vacuum through cryogenic coadsorption of
                                   known quantities of electrolyte species (i.e., solvent, ions, and neutral
                                   molecules)  on  a  metal  surface. 88–91   Such  experiments  serve  as  a  simula-
                                   tion,  or  better,  as  a  synthetic  model  of  electrodes.= The  use  of  surface
                                   spectroscopic techniques m¸es it possiblp to determine the coverage and
                                   structure  of  a  synthesized  electrolyte.= The  interfacial  potential  (i.e.,= the
                                   electrode  woÀ=function)  is  measured  using  the  voltaic  cell  technique.= Of
                                   course,  there are reasonable objections  to the UHV technique,  such as too
                                   little water, too low a temperature, too small interfacial potentials, and lack
                                   of control of ionic activities. 89,91
                                       Non-situ and ex sit  studies can provide important information for
                                   understanding the properties of metal/electrolyte interfaces. The applica-
                                   bility  of these  methods  for fundamental  studies  of electrochemistry  seems
                                   to  be  firmly  established.  The  main  differences  between  common  electro-
                                   chemical  and UHV experiments  are the temperature gap  (ca.= 300 vs.= 150
                                   K)  and  the  difference  in  electrolyte  concentration  (very  high  concentra-
                                   tions in UHV experiments). In this respect, experimental research on
                                   double-layer  properties  in  frozen  electrolytes  can  be  treated  as  a  liØ=
                                                          92
                                   between in  situ  experiments.   The  measurements  of  the  woÀ= functions
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