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will result in the following expression of equilibrium constant [ K e ( T )] at any
temperature ( T ):
[V
Cu ] 2
p 2
K e ( T )
(5.75)
P 1/2
O 2
Furthermore, the validity of the following charge neutrality condition at the outer
interface of the oxide layer suggests
[V
Cu ]
p
(5.76)
So Eq. 5.75 simplifies to
P 1/2
O 2
[V
Cu ] 4
K e ( T )
or
[V
Cu ]
P 1/8
O 2
(5.77)
Since virtual electronic current equilibrium prevails in the oxide layer, migration
of Cu ions through vacant cation sites will become rate limiting for subsequent
thickening of Cu 2 O scale on copper substrate in oxygen atmosphere.
In the expression of Wagner's equation (5.64) for rate constant, since t 1
t Cu
t 3
t h
1 and t 2
t O 2
0 (almost stationary oxygen sublattice),
|
P 1/8
O 2
(theoretical). However, experimentally obtained parabolic rate constants exhibit
the following oxygen pressure dependence relation:
Z O 2
|
2; therefore, one may write
σ
t Cu σ Cu σ
0
Cu ( P O 2
1 atm)
P 1/7
O 2
k r
(Wagner and Gr ¨ newald [18] at 1273 K).
Subsequent studies at 1123 K by Ananth et al. [21-23] have confirmed the valid-
ity of this relation. In either investigation, with plots of k r vs. P 1/7
O 2
when extrapo-
lated to k r
0, the corresponding values of P O 2 agree quite well with the equilib-
rium P O 2 at the Cu-Cu 2 O interface calculated from thermodyamic data, lending
support to the defect model as proposed by Wagner and coworkers [18] for
Cu-Cu 2 O-O 2 (g) system.
Slight deviation from theoretically expected pressure dependence relation
( k r
O 2 ) has been attributed to the presence of some neutral vacancies (V Cu )
along with singly charged vacancies whose concentration predominates over the
concentration of neutral vacancies. However, observation of k r
P 1/8
P 1/4
O 2 by Mrowec
[24,25] has been attributed to a predominance of neutral vacancies in the Cu 2 O
lattice that is not in accord with reports by Wagner et al. [18], Ananth et al. [21-
23], and Bose et al. [26,27]. Reasons for the discrepancy have been elaborated
in recent publications [21-23,26,27].
Similar oxygen pressure dependence of rate constants can also be assumed as
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