Abstract
In part II the moments
v
n
¯
and the low-frequency expansions of lattice frequency distributions were obtained by analyzing experimental heat capacities. We now derive from thermal expansion data the volume dependence of the moments and of the low-frequency coefficients, analyzing the Grüneisen function
γ
(
T
,
V
)
=
β
V
/
χ
s
C
p
. The volume dependence of the moments and of
Θ
0
C
is conveniently expressed by the function
γ
(
n
)
=
−
dln
v
D
(
n
)
/
d
ln
V
, where
v
D
(
n
)
=
1
2
(
n
+
3
)
v
n
¯
1
/
n
. Individual values of γ(
n
) obtained by the analysis are useful in estimating the volume dependence of various crystal properties, notably
C
V
and the Debye-Waller effect. The analysis is carried out for NaCl and KCl. The volume dependence of the low-frequency expansion can in principle be obtained from low-temperature data, but experimental accuracy in fact allows an estimate only of γ
0
≡ γ( — 3); the results are thus wholly expressed by γ(
n
) curves for each salt. These curves are determined to within a few parts per cent for — 2 ≤
n
≤ 0, but the uncertainty increases to about 10% for γ( — 3). For
n
> 0 the uncertainty increases so rapidly that the curves in this range must be considered as only provisional ; this is partly because present thermodynamic data fix the volume dependence of γ(
T, V
) only between very wide limits. The values obtained for y( —3) agree moderately well with values estimated from the pressure dependence of elastic constants; the comparison neither confirms nor rules out the possibility of at least a shallow minimum in the γ(
T
) curves at low temperatures. The general shape of the γ(
n
) carves is in rough agreement with the predictions of the Kellerman rigid ion model, with a maximum in γ(
n
) for
n
> 2. For the Kellerman model the fall in γ(
n
) as
n
→ ∞ is shown to be due to the longitudinal optical modes, which at the long-wave limit have individual γ values lower than γ(2) or γ(4). The primary
C
P
data for sodium chloride of Morrison & Patterson (1956) are tabulated in an appendix, because they were not given in the original paper.
Reference2 articles.
1. B a rro n T . H . K . 1955 P hil.
2. B a rro n T . H . K . 1957 A n n . P hys. 1 77. M a g . 46 720.
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