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Modern Engineering Thermodynamics

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110 CHAPTER 4: The First Law of <strong>Thermodynamics</strong> and Energy Transport Mechanisms<br />

EXAMPLE 4.3 (Continued )<br />

Solution<br />

Let the system be the material inside the tank. The process of<br />

heating the tank is one of constant volume (the tank is “rigid”).<br />

Therefore, since the system volume, V, is constant, dV = 0 and<br />

the moving boundary work is:<br />

p 1 = 0.100 MPa<br />

T 1 = 20°C<br />

Heated sealed<br />

rigid container<br />

Work = ?<br />

p 2 = 0.800 MPa<br />

ð 1<br />

W 2 Þ moving<br />

=<br />

boundary<br />

Z 2<br />

1<br />

pdV = 0<br />

Therefore, no moving boundary work occurs during this process.<br />

FIGURE 4.6<br />

Example 4.3.<br />

State 1 State 2<br />

Since a “rigid” container cannot change its volume, its moving boundary work is always zero regardless of the<br />

process it undergoes.<br />

EXAMPLE 4.4<br />

The weather balloon in Figure 4.7 is inflated from a constant pressure, compressed gas source at 20.0 psia. Determine the<br />

moving system boundary work as the balloon expands from a diameter of 1.00 ft to 10.0 ft.<br />

Solution<br />

<br />

Assume the balloon is a sphere, then V = 4 3 πR 3 = 1 6 πD 3 . The process here<br />

is one of constant pressure, so p = constant, and<br />

p 1 = 20.0 psia<br />

p 2 = 20.0 psia<br />

ð 1<br />

W 2 Þ moving<br />

=<br />

boundary<br />

Z 2<br />

1<br />

pdV = p<br />

Z 2<br />

<br />

= 20:0 lbf 144 in<br />

2<br />

in 2 ft 2<br />

= 1:51 × 10 6 ft.lbf<br />

1<br />

dV = pðV 2<br />

− V 1<br />

Þ<br />

<br />

π<br />

6<br />

<br />

½ð10:0 3 − 1:00 3 Þ ft 3 Š<br />

The work is positive because the balloon does work on the atmosphere as<br />

it expands and pushes the atmosphere out of the way.<br />

D 1 = 1.00 ft dia<br />

D 2 = 10.0 ft dia<br />

State 1 State 2<br />

FIGURE 4.7<br />

Example 4.4.<br />

Exercises<br />

7. In Example 4.3, is the moving boundary work always zero for a sealed, rigid container? Are any other work modes<br />

always zero for this type of system? Could a piston-cylinder apparatus be modeled as a sealed, rigid system? Answers:<br />

Yes, no, no. (It is sealed and the components, the piston and the cylinder, are rigid, but the piston can move, producing<br />

a change in the enclosed volume.)<br />

8. Determine the moving boundary work for the balloon in Example 4.4 as it deflates from a diameter of 10. ft to a diameter<br />

of 5.0 ft at a constant pressure of 20. psia. What does the work on the balloon? Answer:( 1 W 2 ) moving boundary = –1.3 ×<br />

10 6 ft · lbf. The surrounding atmosphere does work on the balloon as it deflates, that is why the work is negative.<br />

9. If the pressure inside a system depends on volume according to the relation p = K 1 + K 2 V + K 3 /V, where K 1 , K 2 , and K 3<br />

are constants, determine the appropriate equation for the moving boundary work done as the volume changes from<br />

V to V : Answer: ð 1 2<br />

1W 2 Þ moving boundary = K 1 ðV − V Þ + K 2 ðV 2 − 2 1 2 V2Þ/2 + K 3 ln ðV /V Þ:<br />

1 2 1<br />

To carry out the integration indicated in Eq. (4.26), the exact p = pðVÞ pressure volume function must be<br />

known. This function is usually given in the process path specification of a problem statement. For example, in<br />

Example 4.3, the process is one of constant volume (the container is rigid), so dV = 0; and in Example 4.4, the<br />

filling process is isobaric (p = constant), so the integral of Eq. (4.26) is very easy. In general, outside of these<br />

two cases, the integration of Eq. (4.26) is not trivial and must be determined with great care.<br />

As an example of a nontrivial integration of Eq. (4.26), consider a process that obeys the relation<br />

pV n = constant (4.27)

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