Solution
Solution
Solution
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12.116<br />
Borgnakke and Sonntag<br />
A Brayton cycle has a compression ratio of 15:1 with a high temperature of<br />
1600 K and an inlet state of 290 K, 100 kPa. Use cold air properties to find the<br />
specific net work output and the second law efficiency if we neglect the “value”<br />
of the exhaust flow.<br />
Brayton cycle so this means:<br />
Minimum T: T 1 = 290 K<br />
Maximum T: T 3 = 1600 K<br />
Pressure ratio: P 2/P 1 = 15<br />
Solve using constant C P0<br />
Compression in compressor: s 2 = s 1 ⇒ Implemented in Eq.8.32<br />
k-1<br />
T2 = T k 0.286<br />
1(P2/P1) = 290(15) = 628.65 K<br />
Energy input is from the combustor<br />
T<br />
2<br />
1<br />
P<br />
3<br />
4<br />
P = 100 kPa<br />
s<br />
q H = h 3 − h 2 = C P0(T 3 − T 2) = 1.004 (1600 − 628.65) = 975.2 kJ/kg<br />
Do the overall cycle efficiency and net work<br />
η = W.<br />
Q .<br />
net<br />
H<br />
= wnet q<br />
= 1 − r<br />
H -(k-1)/k<br />
= 1 − 15<br />
p<br />
-0.4/1.4 = 0.5387<br />
w NET = η q H = 0.5387 × 975.2 = 525.34 kJ/kg<br />
Notice the q H does not come at a single T so neglecting external irreversibility<br />
we get<br />
Φ qH = increase in flow exergy = ψ 3 − ψ 2 = h 3 − h 2 − Τ o (s 3 − s 2 )<br />
= q H − Τ o C P ln(T 3/T 2) = 975.2 – 298.15 × 1.004 ln ( 1600<br />
628.65 )<br />
= 695.56 kJ/kg<br />
ηII = wnet =<br />
ψ3 − ψ2 525.34<br />
695.56<br />
= 0.755<br />
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