IX. THERMAL EXPANSIVITY OF SOLIDS
IX. THERMAL EXPANSIVITY OF SOLIDS
IX. THERMAL EXPANSIVITY OF SOLIDS
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INTRODUCTION TO <strong>THERMAL</strong> <strong>EXPANSIVITY</strong> <strong>OF</strong> <strong>SOLIDS</strong><br />
Values of thermal expansion are given in the form of<br />
(a) total fractional expansion, L293 - LT : and (b) by coefficient<br />
7<br />
L 293<br />
of expansion dL change per unit length per K. For example<br />
L dT ’<br />
the total fractional expansion (or contraction) for copper for<br />
a temperature change from 293.15OK (2OoC) to 50°K is .00321<br />
in./ine, i.e., a bar will be .00321 inches shorter at 50°K-.per<br />
inch of length than it was at 293.15 OK. However, the co-<br />
efficient of expansion for copper at 50 0 K is.0000038 in./in.- 0 K,<br />
i.e. it will expand (or contract) .0000038 inches per inch per<br />
0<br />
0 K temperature change from 50 K.<br />
Reprinted from WADD TECH. REPORT 60-56<br />
. . . .. . . - _. .- . ....<br />
<strong>IX</strong>-A-1<br />
0<br />
January 9, 1967