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Modern Engineering Thermodynamics

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s − s 0 = c ln T T 0<br />

10.8 Flow Availability 333<br />

Solution<br />

First, draw a sketch of the system (Figure 10.11).<br />

3.00 ft/s<br />

T = 50.0°F<br />

4.00 ft<br />

Ground state:<br />

T 0 = 70.0°F<br />

p 0 = 14.7 psia<br />

FIGURE 10.11<br />

Example 10.6.<br />

The unknown is the specific flow availability at the exit of a garden hose. The material is water, and the system is open.<br />

The specific flow availability is defined by Eq. (10.16) as<br />

a f = h − h 0 − T 0 ðs − s 0 Þ + V2<br />

2g c<br />

+ gZ<br />

g c<br />

The liquid water exiting the garden hose fits our definition of an incompressible fluid, so Eqs. (3.62) and (7.33) can be used<br />

to compute<br />

and<br />

h − h 0 = cðT − T 0 Þ + vðp − p 0 Þ<br />

<br />

<br />

Using the subscript w for the water, we can write the specific flow availability of the stream of water exiting the garden<br />

hose as<br />

<br />

ða f Þ w = c w ðT w − T 0 Þ + v w ðp w − p 0 Þ − c w T 0 ln T w<br />

+ V2 w<br />

+ gZ w<br />

T 0 2g c g c<br />

where T 0 = T air = 70.0°F and p 0 = p air = 14.7 psia. The liquid water is a slightly compressed liquid; however, the amount of<br />

compression is only a few psia (p actual − p sat (50.0°F) = 14.7 − 0.1780 = 14.52 psia), and the effect of this small amount of<br />

compression is negligible. Thus, for the specific volume v we use the value of saturated liquid at the actual temperature of<br />

the water, or v = v sat (50.0°F) = 0.01602 ft 3 /lbm. Substituting in all the appropriate numerical values into the specific flow<br />

availability equation, we get<br />

<br />

a f = ð1:00 Btu/lbmÞð50:0 − 70:0RÞ + 0:01602 ft 3 /lbmÞð14:7 − 14:7 lbf/in 2 144 lbf/in 2 <br />

Þ<br />

778:16 ft .lbf/Btu<br />

<br />

<br />

− ð70:0 + 459:67 RÞ ln<br />

50:0 + 459:67<br />

ð3:00 ft/s 2 Þ 2<br />

+<br />

70:0 + 459:67 2ð32:174 lbm.ft/lbf .s 2 Þð778:16 ft .lbf/BtuÞ<br />

ð32:174 ft/s 2 Þð4:00 ftÞ<br />

+<br />

ð32:174 lbm.ft/lbfgs 2 Þð778:16 ft .lbf/BtuÞ = 0:393Btu/lbm<br />

Exercises<br />

16. Determine the value of the flow availability in Example 10.6 when the garden hose is lying on the ground. Assume that<br />

the other variables remain unchanged. Answer: (a f ) w = 0.388 Btu/lbm.<br />

17. Suppose you put a nozzle on the end of the garden hose in Example 10.6 and increase the velocity of the water leaving the<br />

hose from 3.00 ft/s to 15.0 ft/s. Determine the new flow availability, assuming all the other variables remain unchanged.<br />

Answer: (a f ) w = 0.397 Btu/lbm.<br />

18. While you are spraying the garden hose in Example 10.6, a weather front comes through and lowers the atmospheric<br />

temperature from 70.0°F to50.0°F. Determine the new flow availability assuming all the other variables remain unchanged.<br />

Answer: (a f ) w = 0.00500 Btu/lbm.

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