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Modern Engineering Thermodynamics

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8.3 Systems Undergoing Irreversible Processes 261<br />

EXAMPLE 8.8 A CONTINUATION OF EXAMPLE 5.4, WITH<br />

THE ADDITION SHOWN IN ITALIC TYPE<br />

A food blender has a cutting-mixing blade driven by a 0.250 hp electric motor. The machine is initially filled with 1.00 qt of<br />

water at 60.0°F, 14.7 psia. It is turned on at full speed for 10.0 min. Assuming the entire machine is insulated and the mixing<br />

takes place at constant pressure, determine the temperature of the water and the amount of entropy produced when the<br />

machine is turned off.<br />

Solution<br />

First, draw a sketch of the system (Figure 8.8).<br />

The unknowns here are T 2 and l (S P ) 2 . The system is the water in the<br />

blender, which we assume to be an incompressible material. The<br />

data for the water are as follows:<br />

State 1<br />

p 1 = 14:7psia<br />

T 1 = 60:0°F<br />

Isobaric<br />

ƒƒ!<br />

mixing<br />

State 2<br />

p 2 = p 1 = 14:7psia<br />

The solution to the first part of this problem is given in Example 5.4<br />

as m = 2.08 lbm and T 2 =111°F.<br />

The solution to the second part is determined by the indirect method.<br />

Equation (8.1) gives<br />

Z <br />

dQ<br />

1ðS P Þ 2 = ms ð 2 − s 1 Þ−<br />

T b<br />

Σ<br />

1.00 quart of water<br />

System boundary<br />

1 (S P ) 2 = ?<br />

0.250 hp electric motor<br />

and, for an incompressible substance,<br />

so that<br />

s 2 − s 1 = c ln T 2<br />

T 1<br />

0 ðinsulated systemÞ<br />

FIGURE 8.8<br />

Example 8.8.<br />

or<br />

1ðS P Þ 2 = mc ln T 2<br />

T 1<br />

1ðS P<br />

Þ 2 = ð2:08 lbmÞ½1:0 Btu/ ðlbm⋅RÞŠln = 0:195 Btu/R<br />

111 + 459:67<br />

60:0 + 459:67<br />

If we wished to know the entropy production rate for this example, our analysis and results would be the same<br />

as that for part b of Example 8.6. The entropy production rate would not be constant in time, but would<br />

decrease as the water became hotter. Since it is stated that the blender is insulated, eventually enough mixing<br />

energy would be converted into internal (thermal) energy to cause the water to completely vaporize, whereupon<br />

the assumption of an incompressible fluid no longer applies.<br />

EXAMPLE 8.9 A CONTINUATION OF EXAMPLE 5.5, WITH<br />

THE ADDITION SHOWN IN ITALIC TYPE<br />

A new radiation heat transfer sensor consists of a small, closed, rigid, insulated 0.0400 m 3 box containing a 0.0100 m 3<br />

rubber balloon. Initially, the box is evacuated but the balloon contains argon (an ideal gas) at 20.0°C and 0.0100 MPa.<br />

When the balloon receives 0.100 kJ of radiation energy through an uninsulated window in the box, it bursts. The resulting<br />

pressure change is sensed by a pressure transducer and an alarm is sounded. Determine the pressure and temperature inside<br />

the box after the balloon bursts and the entropy produced during this process if the average surface temperature of the heat transfer<br />

window is 400.K.<br />

Solution<br />

First, draw a sketch of the system (Figure 8.9).<br />

(Continued )

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