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

Rh {| align="center" class="wikitable" style="width:80%; text-align:center; margin: 1em auto 1em auto; font-size: 90%;" ! width="5%" | Tempera&shy;tures. ! width="15%" | Volumes to be described by the piston, to complete the fourth operation. ! width="15%" | Volumes from the primitive position of the piston to those occupied at instants of the second operation. ! width="15%" | 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
 * }
 * 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
 * }
 * 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
 * }
 * 220 ||   0.3310. W || x'+ .003130. H || 48512.4
 * 230 ||       0         || x'+ .002643. H || 58376.6
 * }
 * 230 ||       0         || x'+ .002643. H || 58376.6
 * }

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