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12.43<br />

Borgnakke and Sonntag<br />

Consider an ideal air-standard cycle for a gas-turbine, jet propulsion unit, such as<br />

that shown in Fig. 12.9. The pressure and temperature entering the compressor are<br />

90 kPa, 290 K. The pressure ratio across the compressor is 14 to 1, and the turbine<br />

inlet temperature is 1500 K. When the air leaves the turbine, it enters the nozzle<br />

and expands to 90 kPa. Determine the velocity of the air leaving the nozzle.<br />

<strong>Solution</strong>:<br />

1<br />

2 3<br />

BURNER<br />

COMPR. TURBINE<br />

4<br />

NOZ<br />

5<br />

T<br />

2<br />

1<br />

P<br />

3<br />

4<br />

5<br />

P = 90 kPa<br />

C.V. Compressor: Reversible and adiabatic s 2 = s 1 From Eq.8.25, 8.32<br />

T 2 = T 1⎝ ⎜ ⎛<br />

k-1<br />

P2 P1 ⎞ k 0.2857<br />

⎟ = 290 (14) = 616.4 K<br />

⎠<br />

w C = h 2 - h 1 ≈ C P0 (T 2 – T 1) = 1.004 (616.4 – 290) = 327.7 kJ/kg<br />

C.V. Turbine: w T = h 3 - h 4 = w C and s 4 = s 3 ⇒<br />

T 4 = T 3 - w C/C P0 = 1500 - 327.7/1.004 = 1173.6 K<br />

C.V. Nozzle: s 5 = s 4 = s 3 so from Eq.8.32<br />

T 5 = T 3 ⎝ ⎜ ⎛<br />

k-1<br />

P5 P3 Now the energy equation<br />

⎞ k<br />

⎟ = 1500 ⎜<br />

⎠ ⎝ ⎛ 90 ⎞<br />

1260<br />

⎟<br />

⎠<br />

0.2857<br />

= 705.7 K<br />

(1/2)V 5 2 = h4 - h 5 ≈ C P0 (T 4 – T 5) = 1.004 (1173.6 – 705.7) = 469.77 kJ/kg<br />

⇒ V 5 = 2 × 1000 × 469.77 = 969 m/s<br />

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s

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