Abstract
The thermal expansion of copper has been determined at temperatures down to 2 °K by means of an electrical capacitance technique. By measuring three-terminal capacitances in a ratio-transformer bridge length changes smaller than 10
-9
cm can be detected in the capacitor-expansion cell. Below 10 °K, the linear expansion coefficient,
α
, may be represented by
α
= (1·4
5
± 0·1
5
) x 10
-10
T
+ (2·8 ± 0·1) x 10
-11
T
3
per degK. These terms, identified respectively as electronic (
e
) and lattice (
l
) in origin, lead to the following values of the Grüneisen parameter:
γ
e
= 0·63 ± 0·06,
γ
l
= 1·72 ± 0·03 ( =
γ
o
).
γ
e
is compared with a theoretical free-electron value of 2/3, and the low temperature value of
γ
l
is compared with values of 1·75 to 1·77 calculated from elastic constants. At room temperature
γ
(≈ γ
∞
) is 2·00, so that
γ
∞
–
γ
0
≈ 0·28, which agrees well with the theoretical estimates of Barron for a close-packed cubic lattice.
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