Question 15.7: (a) Calculate the work output of a Carnot engine operating b...

(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? (See Figure 15.35.)

Strategy
In both parts, we must first calculate the Carnot efficiency and then the work output.

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Solution (a)
The Carnot efficiency is given by

E f f_{ C }=1-\frac{T_{ c }}{T_{ h }}.                    (15.53)

Substituting the given temperatures yields

E f f_{C}=1-\frac{100 K }{600 K }=0.833.                (15.54)

Now the work output can be calculated using the definition of efficiency for any heat engine as given by

E f f=\frac{W}{Q_{ h }}.                   (15.55)

Solving for W and substituting known terms gives

W=E f f_{ C } Q_{ h }                      (15.56)

= (0.833)(4000 J) = 3333 J.

Solution (b)
Similarly,

E f f_{ C }^{\prime}=1-\frac{T_{ c }}{ T _{ c }^{\prime}}=-\frac{100 K }{250 K }=0.600                    (15.57)

so that

W=E f f^{\prime}{ }_{C} Q_{h}                        (15.58)

= (0.600)(4000 J) = 2400 J.

Discussion
There is 933 J less work from the same heat transfer in the second process. This result is important. The same heat transfer into two perfect engines produces different work outputs, because the entropy change differs in the two cases. In the second case, entropy is greater and less work is produced. Entropy is associated with the unavailability of energy to do work.

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