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Ideal Brayton cycle work and efficiency

Short answer

Using isentropic relations: T2=300×8^0.2857=543.4 K, T4=1200/8^0.2857=662.5 K. Compressor work 244.7 kJ/kg, turbine work 540.2 kJ/kg, net work 295.6 kJ/kg, power 1478 kW, thermal efficiency 44.8%, back work ratio 0.453.

An ideal Brayton cycle takes in air at 100 kPa and 300 K. The pressure ratio is 8 and the maximum cycle temperature is 1200 K. The mass flow rate is 5 kg/s. Taking cp=1.005c_p = 1.005 kJ/kg K and γ=1.4\gamma = 1.4, find (a) the temperatures at all cycle points, (b) the compressor and turbine work, (c) the net work and power, (d) the thermal efficiency and (e) the back work ratio.

(γ−1)/γ=0.2857(\gamma-1)/\gamma = 0.2857 and rp0.2857=80.2857=1.8114r_p^{0.2857} = 8^{0.2857} = 1.8114.

(a) Temperatures

T2=T1rp0.2857=300×1.8114=543.4 K,T4=T3rp0.2857=12001.8114=662.5 KT_2 = T_1 r_p^{0.2857} = 300 \times 1.8114 = 543.4\ \text{K}, \qquad T_4 = \frac{T_3}{r_p^{0.2857}} = \frac{1200}{1.8114} = 662.5\ \text{K}
Point1234
T (K)300543.41200662.5

(b) Compressor and turbine work

wc=cp(T2−T1)=1.005×243.4=244.7 kJ/kgw_c = c_p (T_2 - T_1) = 1.005 \times 243.4 = 244.7\ \text{kJ/kg} wt=cp(T3−T4)=1.005×537.5=540.2 kJ/kgw_t = c_p (T_3 - T_4) = 1.005 \times 537.5 = 540.2\ \text{kJ/kg}

(c) Net work and power

wnet=wt−wc=540.2−244.7=295.6 kJ/kg,P=5×295.6=1478 kWw_{net} = w_t - w_c = 540.2 - 244.7 = 295.6\ \text{kJ/kg}, \qquad P = 5 \times 295.6 = 1478\ \text{kW}

(d) Thermal efficiency

qin=cp(T3−T2)=1.005×656.6=659.8 kJ/kg,η=wnetqin=0.448q_{in} = c_p (T_3 - T_2) = 1.005 \times 656.6 = 659.8\ \text{kJ/kg}, \qquad \eta = \frac{w_{net}}{q_{in}} = 0.448

Check: 1−1/80.2857=0.4481 - 1/8^{0.2857} = 0.448.

(e) Back work ratio

BWR=wcwt=244.7540.2=0.453\text{BWR} = \frac{w_c}{w_t} = \frac{244.7}{540.2} = 0.453

Answer: T2=543.4T_2 = 543.4 K, T4=662.5T_4 = 662.5 K; wc=244.7w_c = 244.7, wt=540.2w_t = 540.2, wnet=295.6w_{net} = 295.6 kJ/kg; P=1478P = 1478 kW; η=44.8%\eta = 44.8\%; BWR = 0.453.

✓ Answer checked by Claude Opus 5.5 (high effort)

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