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62                                                    O.F.  Putikov and B.  Wen

                 T     .... ...i  ;2   I   13
                    ~
                     9
                                      1
                                      ............ i
                                     I  i
                  ,t__  .....  .x.   I   /

             4""  ~i ./"  "'~,  l~.]".."  i /"




                   0      q)l   (P2   q)3
           Fig.  2-40.  Influence  of  linear  disturbances  on  the  shape  of  the  polarisation  curve:  I-  ideal
           polarisation  curve;  2-  linear  disturbances  with  inadequate  compensation;  3-  polarisation  curve
           under  condition  of inadequate  compensation  of  linear  disturbances;  4-  linear  disturbances  with
           over-compensation;  5-  polarisation  curve  under  condition  of  over-compensation  of  linear
           disturbances (reproduced  with permission from Putikov,  1993).



           ~AU~ disturbance.  To  do  this  a  compensation  voltage  AUcom  is  applied  to  the  measuring
           potential  set.  The  compensation  voltage  Ucom is  proportional  to  the  current,  but  has  an
           opposite  sign  to  the  voltage  ZAU~.  The  compensation  voltage  is  taken  from  a  special
           resistor (3)  in the  current  circuit (Fig.  2-39).  Then  at the measuring  potential  set  inlet we
           have,


           AU r,,~ -  AU MN  +  AU :or.  -  ~n +  ~  AU  ;  +  AU :or.  -  ~  + a ( A U )


           where  AUmes  is  the  measuring  voltage  and  6(AU)  is  the  disturbance  voltage,  which  is  a
           linear  function  of current.  In  the  case  of  full  compensation  5(AU)  =  0,  ZAU~ =  -AUcom
           and  AUmes  -  q).  For  proper  compensation  it  is  necessary  to  change  the  compensation
           resistor  value,  then  we  obtain  an  ideal  polarisation  curve  (Fig.  2-40,  curve  1).  With
           inadequate  compensation  or  over-compensation  we  obtain  distorted  polarisation  curves
           (Fig.  2-40,  curves  3,  5).  It  is  not  essential  to  achieve  full  compensation  of disturbances
           for  the  satisfactory  determination  of  the  electrochemical  reaction  potentials  (q)l,  q)2  ...)
           and  corresponding  limiting  currents  (Iliml,  Ilim2 ...).  Using  polarisation  curves  with  some
           inadequate  compensation  or with  some  over-compensation  may even be  successful.  The
           compensation  operation  is  necessary  only  for  good  representation  of  the  polarisation
           wave  steps.
              The current source  and current circuit must also satisfy definite  requirements  (Ryss et
           al.,  1978:  Ryss,  1973),  including:  (1)  the  possibility  to  change  the  current  over  time  in
           different  ways  up  to  the  maximum  values  (160-250  A);  and  (2)  minimal  resistance  in
           the  current  circuit  (including  cable,  electrode  A,  electrode  B  and  all  other  parts).  For
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