IX. THERMAL EXPANSIVITY OF SOLIDS
IX. THERMAL EXPANSIVITY OF SOLIDS
IX. THERMAL EXPANSIVITY OF SOLIDS
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Sources of Data:<br />
Other References<br />
Discussion:<br />
Temp.<br />
0<br />
K<br />
0<br />
5<br />
10<br />
20<br />
30<br />
40<br />
50<br />
60<br />
70<br />
80<br />
90<br />
100<br />
Taken<br />
L<br />
293 - LT<br />
708<br />
708<br />
707<br />
700<br />
68 6<br />
667<br />
64 6<br />
624<br />
60 1<br />
5 77<br />
552<br />
5 28<br />
L293<br />
I1<br />
I1<br />
I1<br />
11<br />
I1<br />
II<br />
I1<br />
I1<br />
II<br />
I1<br />
I1<br />
from NBS 29<br />
<strong>THERMAL</strong> EXPANSION <strong>OF</strong> LEAD<br />
Dheer and Surange 1958, Ebert 1928, Nix and<br />
MacNair 1942, Olsen and Rohrer 1957.<br />
Dorsey 1908, Gruneisen 1910, Head and L que r<br />
1952, Lindemann 1911, McLennan, Allen and<br />
Wilhelm 1931.<br />
Superconducting lead has a slightly greater<br />
volume and a slightly smaller expansion coefficient<br />
than normal lead according to data by<br />
Olsen and Rohrer covering the region from lo<br />
to the transititon temperature, 7.2OK. For<br />
example, the difference in expansion coefficients<br />
at 5OK is about 10%.<br />
Table of Selected Values<br />
-- 1 dL Temp.<br />
0 L293 - LT -- 1 dL<br />
L dT<br />
K<br />
L dT<br />
per OK<br />
L293 per OK<br />
0<br />
0.03<br />
0.32 I'<br />
1.1 II<br />
1.7<br />
I1<br />
2 .o<br />
I1<br />
2.2<br />
I1<br />
2.3<br />
II<br />
2.4<br />
I1<br />
2.4<br />
I1<br />
2.5 II<br />
2.5<br />
I1<br />
120<br />
140<br />
160<br />
180<br />
200<br />
220<br />
240<br />
2 60<br />
273<br />
280<br />
2 93<br />
300<br />
<strong>IX</strong>-M- 1.<br />
477<br />
425<br />
I1<br />
372 I1<br />
318<br />
I1<br />
2 63<br />
I1<br />
208<br />
I1<br />
15 2 II<br />
96<br />
11<br />
58<br />
I1<br />
38<br />
0<br />
-20<br />
I1<br />
2.56 x<br />
2.63<br />
2.68<br />
2.72<br />
2.75<br />
2.78<br />
2.82<br />
2.85<br />
2.88<br />
2.89<br />
2.9<br />
2.9<br />
I1<br />
II<br />
I1<br />
II<br />
I1<br />
11<br />
I1<br />
II<br />
I1<br />
I1<br />
I1