Abstract
On elementary theories, the ionic current
i
through the oxide is expected in the steady state to depend on the field strength
E
in the oxide (as measured by oxide overpotential/thickness of oxide) and the temperature
T
according to an equation of the form
i
=
i
0
exp { – (
W
–
qaE
)/
kT
}, where
i
0
,
W
and
a
are constants which have different significance according to the model,
q
is the charge on the ion, and
k
is Boltzmann’s constant. The relation has been investigated experimentally by a spectrophotometric method of determining the thickness of the oxide. It was found that the experimental results for dilute solutions could be represented within less than 1 % of
E
at 2490 Ả thickness by the above equation with
qaE
replaced by
q
(α + β
E
)
E
where α and β are constants with
i
0
= 10
8.24
A/cm
2
,
W
= 2.185 eV, α = 6.995Ả,β = – 3.35Ả/(10
7
V/cm) and
q
= 5
e
. The modifications that occur as the concentration of acid is increased have been investigated. In concentrated acid, although less charge is required to form a film of given optical thickness, the films have a lower a.c. capacity, and require a higher overpotential to produce a given ionic current density. The capacity of films formed to a given overpotential at a given current density is almost independent of the concentration of the acid. The significance of the results is discussed in connexion with how far the existence of a range of site parameters (in particular, activation energy and activation distance) in an amorphous oxide tends to explain them, or whether a more fundamental change in the equations used to describe ionic movement is required.
Reference11 articles.
1. Bean C. R . Fisher J . C. & V erm ilyea D. A. 1956 Rev. 101 551.
2. Cabrera N. & M ott N. F . 1948 Rep.
3. Dewald J . F . 1955 J .
4. Phys. 12 163. Electrochem.Soc. 102 1.
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