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Modern Engineering Thermodynamics

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4.6 Mechanical Work Modes of Energy Transport 109<br />

L<br />

Area A<br />

p<br />

F<br />

± F<br />

x<br />

dx<br />

Area A<br />

x<br />

± dx<br />

(a) Moving system boundary<br />

(c) Elastic work<br />

Wire frame<br />

T<br />

dΘ<br />

b<br />

x<br />

Film<br />

± dx<br />

± F<br />

Moving slider<br />

(b) Shaft work<br />

(d) Surface tension work<br />

FIGURE 4.5<br />

Four classical types of mechanical work.<br />

or<br />

ð 1<br />

W 2 Þ mechanical<br />

=<br />

Z x2<br />

x1<br />

ð F ! applied by the system Þ .d x ! −<br />

Z x2<br />

x1<br />

ð F ! applied on the system Þ .d x ! (4.24)<br />

Note that our sign convention requires that work done by the system be positive, while work done on the system<br />

be negative.<br />

In thermodynamics, the four classical types of mechanical work (Figure 4.5) are<br />

1. Moving system boundary work.<br />

2. Rotating shaft work.<br />

3. Elastic work.<br />

4. Surface tension work.<br />

These are very important work modes in engineering analysis and the following material provides a detailed<br />

discussion of their major characteristics.<br />

4.6.1 Moving System Boundary Work<br />

Whenever a system boundary moves such that the total volume of the system changes, moving system boundary<br />

work occurs. This is sometimes called expansion or compression work, and it has wide application in mechanical<br />

power technology. In this case, the force is applied by the system through the pressure p (see Figure 4.5a), so<br />

! ! !<br />

F = p A and F . d ! x = pA ! .d ! x = pdV, where p is the pressure acting on the system boundary, ! A is the area vector<br />

(defined to be normal to the system boundary and pointing outward), d ! x is the differential boundary movement,<br />

and dV is the differential volume ! A .d ! x : Consequently,<br />

and for moving boundary work,<br />

ðdWÞ moving<br />

= pdV (4.25)<br />

boundary<br />

Moving boundary work:<br />

ð 1<br />

W 2 Þ moving<br />

boundary<br />

=<br />

Z 2<br />

1<br />

pdV (4.26)<br />

EXAMPLE 4.3<br />

The sealed, rigid tank shown in Figure 4.6 contains air at 0.100 MPa and 20.0 °C. The tank is then heated until the pressure<br />

in the tank reaches 0.800 MPa. Determine the mechanical moving boundary work produced in this process.<br />

(Continued )

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