Abstract
When the temperature variation of a saturated thermionic current
i
per unit area is represented by plotting log (
i
/T
2
) against 1/T, it has been customary to identify the slope and the vertical intercept of the graph with the electronic work function
ϕ
and the logarithm of the emission constant A, respectively, in Richardson’s equation
i
= AT
2
e
-
ϕ /k
T
. This identification has been reasonably successful for materials of a high degree of homogeneity, since they exhibit straight “Richardson plots” whose measurement offers values of A and
ϕ
not inconsistent with electronic data from other sources. On the other hand, certain materials exhibit curved plots, indicating at once that no fixed A and
ϕ
can be recorded. Others, with which we are here concerned, give plots which appear straight over an observed range but suggest values of A and
ϕ
, disagreeing so radically with established theory or with indirect experiments that they have been regarded as anomalous. We prove in one instance that an extension of the range reveals such a plot as part of a curve, and that the curve contains implicit quantities not solely electronic and therefore not expressed by even a sequence of simple Richardson equations. Hence the slopes and intercepts of tangents to this curve are not identifiable with values of
ϕ
and log A.
Cited by
10 articles.
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