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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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