Solution
Solution
Solution
You also want an ePaper? Increase the reach of your titles
YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.
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 />
Excerpts from this work may be reproduced by instructors for distribution on a not-for-profit basis for<br />
testing or instructional purposes only to students enrolled in courses for which this textbook has been<br />
adopted. Any other reproduction or translation of this work beyond that permitted by Sections 107 or 108<br />
of the 1976 United States Copyright Act without the permission of the copyright owner is unlawful.<br />
s