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Modern Engineering Thermodynamics

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262 CHAPTER 8: Second Law Closed System Applications<br />

EXAMPLE 8.9 (Continued )<br />

Window<br />

T window = 400. K<br />

Rigid insulated box<br />

with a volume of<br />

0.0400 m 3<br />

Argon-filled balloon<br />

initially with a volume<br />

of 0.0100 m 3 at 20.0°C<br />

and 10.0 kPa<br />

FIGURE 8.9<br />

Example 8.9.<br />

The unknown is the entropy produced during this process if the average surface temperature of the heat transfer window is<br />

400. K. The material is argon gas.<br />

In Example 5.5, we use an energy balance to find the final pressure and temperature as p 2 = 4.15 kPa and T 2 = 214°C = 487 K.<br />

Now, an entropy balance gives<br />

1Q 2<br />

T b<br />

which can be solved for the entropy production as<br />

+ 1 ðS P Þ 2<br />

= mðs 2 − s 1 Þ argon<br />

1ðS P Þ 2 = mðs s − s 1 Þ − 1 Q 2<br />

T b<br />

and, since argon is an ideal gas, we can write<br />

s 2 − s 1 = c p ln ðT 2 /T 1 Þ− R ln ðp 2 /p 1 Þ<br />

From Table C.13b of Thermodynamic Tables to accompany <strong>Modern</strong> <strong>Engineering</strong> <strong>Thermodynamics</strong>, we find that for argon,<br />

c p = 0.523 kJ/kg · KandR =0.208kJ/kg· K; and from Example 5.5, the mass of the argon is m = 0.00164 kg. Then, with<br />

1Q 2 =0.100kJandT b = 400. K, we get<br />

<br />

<br />

<br />

<br />

214 + 273:15 K<br />

4:15 kPa<br />

1ðS P Þ 2 = ð0:00164 kgÞ ð0:523 kJ/kg.KÞ ln<br />

− ð0:208 kJ/kg.KÞln<br />

20:0 + 273:15 K<br />

10:0kPa<br />

0:100 kJ<br />

−<br />

400: K = 0:486 × 10−3 kJ/K = 0:486 J/K<br />

In this example, the heat transfer occurs over only a portion of the system’s surface (the uninsulated window). The rest of<br />

the enclosure is insulated to prevent the sensor from being influenced by anything except the heat source in front of the<br />

window. Though the surface temperature of the window probably changes during the heat transfer process, an adequate<br />

solution is obtained simply by using an average surface temperature during the process of T b = 400. K.<br />

Exercises<br />

14. Suppose the balloon in Example 8.9 is designed to burst after absorbing 0.200 kJ of radiation heat transfer. Determine<br />

the entropy produced during this process if the average surface temperature of the heat transfer window is 500. K.<br />

Answer: 1 (S P ) 2 = 0.336 J/K.<br />

15. If air were substituted for the argon in Example 8.9 with no changes in the remaining parameters, what would be the<br />

entropy produced inside the box during this process? Answer: 1 (S P ) 2 = 0.510 J/K.<br />

16. Determine the entropy produced when the radiation heat transfer is increased to produce a final pressure of 20 kPa in<br />

the box after the balloon bursts. Assume that the average temperature of the heat transfer window is 1200 K for this<br />

process. Answers: 1 (S P ) 2 = 0.664 J/K.<br />

EXAMPLE 8.10 A CONTINUATION OF EXAMPLE 5.6, WITH<br />

THE ADDITION SHOWN IN ITALIC TYPE<br />

Suppose 0.100 lbm of Refrigerant-134a initially at 180.°F and 100. psia in a cylinder with a movable piston undergoes the<br />

following two-part process. First, the refrigerant is expanded adiabatically to 30.0 psia and 120.°F, then it is isobarically compressed<br />

to half its initial volume. Determine<br />

a. The work transport of energy during the adiabatic expansion.<br />

b. The heat transport of energy during the isobaric compression.

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