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has been related to the self-diffusion coefficients, D 1 and D 2 of metal and non-
metal ions, respectively, for an oxide of t e
1. Using Einstein's relation,
D i
drift velocity of species i per unit force; Wagner finally
obtained the following expression for k r :
B i kT , where B i
a (o)
O
a (i)
O
|
Z 1 |
k r
C equiv
D 1
D 2
dln a O
(5.88)
|
Z 2 |
or
a (i M
a (o)
O
D 1 |
Z 2 |
k r
C equiv
D 2
dln a M
(5.89)
|
Z 1 |
where
C equiv
(concentration in kg equivalent of compound)
m 3
D 1 and D 2
self-diffusion coefficient of cations and anions, respectively, in
the compound layer, expressed in m 2
s 1
Z 1 and Z 2
valence of metal and nonmetal atoms, respectively,
a (o) O and a (i O
activity of oxidant at the outer oxide-oxygen and the inner
metal-oxide interfaces, respectively
a (o M and a (i M
activity of metal atoms at the outer oxide-oxygen and the inner
metal-oxide interfaces, respectively
Wagner's theoretical relation (5.88) for parabolic rate constant has been success-
fully tested and found to be valid for a large number of metal-oxidant systems.
However, his expression considered only lattice or volume diffusion in the grow-
ing product layer but did not take into account the diffusion through grain bound-
ary and other easy diffusion paths. In many a situation, porosities and microchan-
nels are developed within the scale where this model is not fully satisfied.
Moreover, no specific mention has been made regarding the temperature of appli-
cability of this theoretical relation. Subsequent experimentations have established
that the temperature of validity of this mechanism will vary from one system to
another.
5.5.2 Determination of Self-Diffusion Coefficient from
Parabolic Rate Constant
Fueki and Wagner (31) and subsequently Pettit (32) evaluated self-diffusion coef-
ficient from the knowledge of oxygen pressure dependence of rational rate con-
stant ( k r ) by following an inverse procedure, i.e., by differentiating Eq. 5.88 as
proposed by Wagner (30), which correlates k r and diffusivity values of ionic
species. One would obtain the following expression by differentiating Eq. 5.88:
 
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