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Modern Engineering Thermodynamics

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326 CHAPTER 10: Availability Analysis<br />

EXAMPLE 10.3<br />

The instrument cooling system on an aircraft flying at 30.0 × 10 3 ft at 500. mph contains 5.00 lbm of saturated liquid<br />

Refrigerant-22 at 50°F. As the aircraft lands, a malfunction occurs that causes the refrigerant to be heated to 400.°F and<br />

100. psia. Determine<br />

a. The total availability of the refrigerant before and after the aircraft lands.<br />

b. The change in total availability during the landing.<br />

Take the local environment (ground state) to be saturated liquid Refrigerant-22 at T 0 = 70.0°F (sothatp 0 = p sat (70.0°F) =<br />

136.12 psia).<br />

Solution<br />

First, draw a sketch of the system (Figure 10.7).<br />

R-22<br />

Ground state:<br />

R-22 at 70.0°F and 136.12 psia<br />

FIGURE 10.7<br />

Example 10.3.<br />

The unknowns are the total availability of the refrigerant before and after the aircraft lands and the change in total availability<br />

during the landing. The material is R-22, and the system is closed.<br />

a. The total availability of a system is given by Eq. (10.3) as<br />

<br />

A = m u − u 0 + p 0 ðv − v 0 Þ − T 0 ðs − s 0 Þ + V2 + gZ <br />

2g c g c<br />

Tables C.9a and C.10a give the thermodynamic properties of the refrigerant as<br />

State 1 ðflyingÞ State 2 ðlandedÞ Ground state<br />

x 1 = 0:00 p 2 = 100:psia x 0 = 0:00<br />

T 1 = 50:0°F T 2 = 400:°F T 0 = 70:0°F<br />

v 1 = 0:01281 ft 3 /lbm v 2 = 1:046 ft 3 /lbm v 0 = 0:01325 ft 3 /lbm<br />

u 1 = 24:04 Btu/lbm u 2 = 154:77 Btu/lbm u 0 = 29:78 Btu/lbm<br />

s 1 = 0:0519 Btu/lbm.R s 2 = 0:31464 Btu/lbm.R s 0 = 0:06296 Btu/lbm.R<br />

V 1 = 500 mph V 2 = 0 p 0 = 136:12 psia<br />

Z 1 = 30,000 ft Z 2 = 0<br />

The total availability is given by Eq. (10.5) as<br />

<br />

A = mu− u 0 + p 0 ðv − v 0 Þ − T 0 ðs − s 0 Þ + V 2 <br />

/2g c + gZ/g c

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