T- 600 K T= 600 K 4000 J T = 250 K Q, 4000 J Entropy increases Q = 4000 J W = 3333 J W = 2400 J 667 J Q. = 1600 J T. = 100 K T = 100 K Carnot engine Greater entropy overall (b) Carnot engine (a) Figure 15.35 (a) A Carnot engine working at between 600 K and 100 K has 4000 J of heat transfer and performs 3333 J of work. (b) The 4000 J of heat transfer occurs first irreversibly to a 250 K reservoir and then goes into a Carnot engine. The increase in entropy caused by the heat transfer to a colder reservoir results in a smaller work output of 2400 J. There is a permanent loss of 933 J of energy for the purpose of doing work.

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(a) Calculate the work output of a Carnot engine operating between temperatures of 600 K and 100 K for 4000 J of heat transfer to the engine.      (b) Now suppose that the 4000 J of heat transfer occurs first from the 600 K reservoir to a 250 K reservoir (without doing any work, and this produces the increase in entropy calculated above) before transferring into a Carnot engine operating between 250 K and 100 K. What work output is produced?

T- 600 K
T= 600 K
4000 J
T = 250 K
Q, 4000 J
Entropy
increases
Q = 4000 J
W = 3333 J
W = 2400 J
667 J
Q. = 1600 J
T. = 100 K
T = 100 K
Carnot engine
Greater entropy overall
(b)
Carnot engine
(a)
Figure 15.35 (a) A Carnot engine working at between 600 K and 100 K has 4000 J of heat transfer and performs 3333 J of work. (b) The 4000 J
of heat transfer occurs first irreversibly to a 250 K reservoir and then goes into a Carnot engine. The increase in entropy caused by the heat
transfer to a colder reservoir results in a smaller work output of 2400 J. There is a permanent loss of 933 J of energy for the purpose of doing
work.
Transcribed Image Text:T- 600 K T= 600 K 4000 J T = 250 K Q, 4000 J Entropy increases Q = 4000 J W = 3333 J W = 2400 J 667 J Q. = 1600 J T. = 100 K T = 100 K Carnot engine Greater entropy overall (b) Carnot engine (a) Figure 15.35 (a) A Carnot engine working at between 600 K and 100 K has 4000 J of heat transfer and performs 3333 J of work. (b) The 4000 J of heat transfer occurs first irreversibly to a 250 K reservoir and then goes into a Carnot engine. The increase in entropy caused by the heat transfer to a colder reservoir results in a smaller work output of 2400 J. There is a permanent loss of 933 J of energy for the purpose of doing work.
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