Page:Reflections on the Motive Power of Heat.djvu/203

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MOTIVE POWER OF HEAT.
171
Tempera­tures. Volumes to be described by the piston, to complete the fourth operation. Volumes from the primitive position of the piston to those occupied at instants of the second operation. Pressures of saturated steam, in pounds on the square foot.
t x' x y = y' = p
0 1269. W x'+5.409. H 12.832
10 639.6. W x'+2.847. H 25.567
20 337.3. W x'+1.571. H 48.514
30 185.5. W x'+ .9062. H 88.007
40 105.9. W x'+ .5442. H 153.167
50 62.62. W x'+ .3392. H 256.595
60 38.19. W x'+ .2188. H 415.070
70 21.94. W x'+ .1456. H 650.240
80 15.38. W x'+ .09962. H 989.318
90 10.09. W x'+ .06994. H 1465.80
100 6.744. W x'+ .05026. H 2120.11
110 4.578. W x'+ .03688. H 2999.87
120 3.141. W x'+ .02758. H 4160.10
130 2.176. W x'+ .02098. H 5663.70
140 1.519. W x'+ .01625. H 7581.15
150 1.058. W x'+ .01271. H 9990.26
160 0.7369. W x'+ .01010. H 12976.2
170 0.5085. W x'+ .008116. H 16630.7
180 0.3454. W x'+ .006592. H 21051.5
190 0.2267. W x'+ .005406. H 26341.5
200 0.1409. W x'+ .004472. H 32607.7
210 0.0784. W x'+ .003729. H 39960.7
220 0.3310. W x'+ .003130. H 48512.4
230 0 x'+ .002643. H 58376.6

Appendix.

(Read April 30, 1849.)

41. In p. 30 some conclusions drawn by Carnot from his general reasoning were noticed; according to which it appears, that if the value of μ for