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for the same potential range and the data are not influenced by the
current offset. One scan rate is taken as a reference, while more
scan rates are chosen as selected multiples of the reference scan
rate.
For elimination procedure, two necessary assumptions must be
fulfilled:
1. The total current resulting from different individual processes
such as diffusion, adsorption, and kinetics is formed by the sum
ofthese particular currents:
I
= I d + I c + I k ,
where I d , I c ,and I k are the diffusion, charging, and kinetic
currents, respectively.
2. The particular currents eliminated are expressed as the product
oftwo independent functions:
= Y j ( E ) W j ( ν ) ,
I j
where Y j ( E )istheelectrodepotentialfunctionand W j ( ν )isthe
scan rate function.
The scan rate function has the form of a certain power of x of the
scan rate. For example, for a substance transported to an electrode
only by diffusion, the rate power coe cient of 1
/ 2 corresponds to
the diffusion current I d , while x = 1 or 0 holds for the charging
current I c ,orthekineticcurrent I k ,respectively[5-7,21].According
to the second condition of the elimination procedure, the particular
currents take the form
Y d ( E ) v 1 / 2
Y k ( E ) v 0
Y c ( E ) v 1
I d =
,
I k =
,
and I c =
,
where Y j ( E ) of the individual current characterizes a proportion-
ality which is independent of scan rate at the selected potential
value. It has been proved that for the elimination function f ( I )in
addition to the total current at a reference scan rate I , the total
currents for half and double of its value, I 1 / 2 and I 2 , are suitable
[5, 7, 13, 21]. EVLS functions have been used for the different
combinationswiththesamescanrateratio(integer2)formorethan
13 years. The types of six elimination functions are presented in
Table 11.1.
 
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