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Modern Engineering Thermodynamics

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218 CHAPTER 7: Second Law of <strong>Thermodynamics</strong> and Entropy Transport and Production Mechanisms<br />

CRITICAL THINKING<br />

Notice that, the smaller the difference between T H and T L , the larger the COP defined in Eqs. (7.18) and (7.20) becomes. To<br />

understand this on a physical basis, note that, since the numerator is a fixed value (Q L or Q H ) in both equations and the<br />

denominator represents the net work input (W in ) to the device, it stands to reason that, the smaller is the work input for a<br />

given output, the better the efficiency (i.e., COP) is.<br />

Comparing Eqs. (7.17) and (7.19), we see that<br />

COP heat pump = COP refrig: or<br />

+ 1<br />

air cond:<br />

EXAMPLE 7.3<br />

The temperature outside on a hot summer day is 95°F. You would like your room to<br />

be at 70.°F, so you go out shopping for an air conditioner. If you are going to buy a<br />

Carnot air conditioner, what should be its coefficient of performance?<br />

(COP) = ?<br />

Carnot<br />

AC<br />

Solution<br />

First, draw a sketch of the system (Figure 7.10).<br />

95.°F<br />

Carnot<br />

air<br />

conditioner<br />

70.°F<br />

The unknown is the coefficient of performance of an air conditioner operating between<br />

70.°F and 95°F. Equation (7.20) gives the coefficient of performance for a Carnot air<br />

conditioner as<br />

COP Carnot<br />

=<br />

refrig: or<br />

air cond:<br />

T L<br />

T H − T L<br />

=<br />

70: + 459:67<br />

ð95 + 459:67Þ − ð70: + 459:67Þ = 21<br />

Note that, in the denominator, the temperature difference in this equation can be in<br />

either relative or absolute temperature units because (95 + 459.67) − (70. + 459.67) =<br />

95 − 70. = 25°F or R. The degree size is the same for both the absolute and the relative<br />

temperature scales.<br />

FIGURE 7.10<br />

Example 7.3.<br />

The coefficient of performance of a real air conditioner is sometimes called its energy efficiency rating (EER) and usually ranges<br />

between 3 and 9. The value of 21 calculated in Example 7.3 is unreasonably high, because a Carnot air conditioner is reversible<br />

and has no friction or other internal losses. Therefore, it requires less input work than a real air conditioner.<br />

Exercises<br />

5. The refrigerator in your kitchen maintains a temperature difference of 2.00°C inside when the outside kitchen<br />

temperature is 22.0°C. If it is a Carnot refrigerator, what is its coefficient of performance? Answer: (COP) Carnot ref. = 13.8.<br />

6. If the Carnot air conditioner purchased in Example 7.3 is inserted into the window backward during the winter and<br />

operated as a heat pump, determine its coefficient of performance as a heat pump. Answer: (COP) Carnot HP = 22.<br />

7.7 CLAUSIUS’S DEFINITION OF ENTROPY<br />

Rudolph Clausius extended Thomson’s absolute temperature scale work by rearranging Eq. (7.15) to read<br />

ðQ H Þ rev<br />

= jQ Lj rev<br />

T H T L<br />

and since this applies only to a closed system undergoing a thermodynamic cycle, it can also be written as<br />

∑<br />

cycle<br />

<br />

Q<br />

T<br />

<br />

= ðQ HÞ rev<br />

T H<br />

− jQ Lj rev<br />

T L<br />

= 0<br />

If we now take an arbitrary thermodynamic closed system cycle and overlay it with an infinite number of<br />

infinitesimal heat engine cycles, as shown in Figure 7.11, then we can extend the finite summation process of<br />

the previous equation into a cyclic integral. Also, since each of these infinite number of heat engines is now

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