120by and the number ofmoles on the left and right sides of thecylinder,
respectively, andusing we obtain the total work and, hence,
heat given by theintegral
4.29 Heat Extraction (MIT, Wisconsin-Madison)
a)For a mass of fixedvolume we haveSo, by the definition ofC,SinceCis independent ofT,we may rewrite (S.4.29.2) andintegrate:The change in entropy isthenb) The maximum heat may be extracted when the entropy remainscon-
stant. Equating theinitial and finalentropies yields thefinaltemperature
of the two bodies:SOLUTIONS