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188
THOMSON ON CARNOT'S
(2) And that the quantity of heat evolved in all circumstances, when the temperature of the gas is given, is proportional to the amount of work spent in the compression.
51. The expression for the amount of work necessary to produce a unit of heat is
and therefore Regnault's experiments on steam are available to enable us to calculate its value for any temperature. By finding the values of μ at 0°, 10°, 20°, etc., from Table I., and by substituting successively the values 0, 10, 20, etc., for t, the following results have been obtained:
Table of the Values of .
| Work requisite to produce a unit of Heat by the compression of a Gas. | Temperature of the Gas. | Work requisite to produce a unit of Heat by the compression of a Gas. | Temperature of the Gas. |
|---|---|---|---|
| Ft.-pounds. | ° | Ft.-pounds. | ° |
| 1357.1 | 0 | 1446.4 | 120 |
| 1368.7 | 10 | 1455.8 | 130 |
| 1379.0 | 20 | 1465.3 | 140 |
| 1388.0 | 30 | 1475.8 | 150 |
| 1395.7 | 40 | 1489.2 | 160 |
| 1401.8 | 50 | 1499.0 | 170 |
| 1406.7 | 60 | 1511.3 | 180 |
| 1412.0 | 70 | 1523.5 | 190 |
| 1417.6 | 80 | 1536.5 | 200 |
| 1424.0 | 90 | 1550.2 | 210 |
| 1430.6 | 100 | 1564.0 | 220 |
| 1438.2 | 110 | 1577.8 | 230 |
