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Actual gas turbine cycle with component efficiencies

Short answer

Considering compressor and turbine efficiencies and 5% pressure loss, T2=528.7 K, T4=751.4 K; net specific work=127.3 kJ/kg; thermal efficiency=20.4%; work ratio=0.345; power=1910 kW.

A gas turbine plant takes in air at 100 kPa and 288 K. The compressor pressure ratio is 6 and its isentropic efficiency is 80%. The pressure loss in the combustion chamber is 5% of the compressor delivery pressure and the turbine inlet temperature is 1073 K. The turbine isentropic efficiency is 85% and it exhausts to 100 kPa. For air cp=1.005c_p = 1.005 kJ/kg K, γ=1.4\gamma = 1.4; for the gases cp=1.148c_p = 1.148 kJ/kg K, γ=1.333\gamma = 1.333. Neglect the mass of fuel. Find (a) the compressor delivery temperature, (b) the turbine exit temperature, (c) the net specific work, (d) the thermal efficiency, (e) the work ratio, and (f) the power for a flow of 15 kg/s.

Data: T1=288T_1 = 288 K, rp=6r_p = 6, ηc=0.80\eta_c = 0.80, ηt=0.85\eta_t = 0.85, T3=1073T_3 = 1073 K, m˙=15\dot m = 15 kg/s.

(a) Compressor

T2s=288×60.2857=480.5 KT_{2s} = 288 \times 6^{0.2857} = 480.5\ \text{K} wc=cp(T2s−T1)ηc=1.005×192.50.80=241.9 kJ/kg,T2=288+241.91.005=528.7 Kw_c = \frac{c_p (T_{2s} - T_1)}{\eta_c} = \frac{1.005 \times 192.5}{0.80} = 241.9\ \text{kJ/kg}, \qquad T_2 = 288 + \frac{241.9}{1.005} = 528.7\ \text{K}

(b) Turbine

Pressure at turbine inlet p3=0.95×600=570p_3 = 0.95 \times 600 = 570 kPa, so the expansion ratio is 570/100=5.70570/100 = 5.70.

γ−1γ=0.2498,T4s=T3rt0.2498=10731.5446=694.7 K\frac{\gamma - 1}{\gamma} = 0.2498, \quad T_{4s} = \frac{T_3}{r_t^{0.2498}} = \frac{1073}{1.5446} = 694.7\ \text{K} wt=ηtcp(T3−T4s)=0.85×1.148×378.3=369.2 kJ/kgw_t = \eta_t c_p (T_3 - T_{4s}) = 0.85 \times 1.148 \times 378.3 = 369.2\ \text{kJ/kg} T4=T3−wtcp=1073−369.21.148=751.4 KT_4 = T_3 - \frac{w_t}{c_p} = 1073 - \frac{369.2}{1.148} = 751.4\ \text{K}

(c) Net work

wnet=wt−wc=369.2−241.9=127.3 kJ/kgw_{net} = w_t - w_c = 369.2 - 241.9 = 127.3\ \text{kJ/kg}

(d) Thermal efficiency

qin=cp,g(T3−T2)=1.148×(1073−528.7)=624.9 kJ/kgq_{in} = c_{p,g} (T_3 - T_2) = 1.148 \times (1073 - 528.7) = 624.9\ \text{kJ/kg} ηth=wnetqin=127.3624.9=0.204\eta_{th} = \frac{w_{net}}{q_{in}} = \frac{127.3}{624.9} = 0.204

(e) Work ratio and (f) power

Work ratio=wnetwt=127.3369.2=0.345(back work ratio=0.655)\text{Work ratio} = \frac{w_{net}}{w_t} = \frac{127.3}{369.2} = 0.345 \quad (\text{back work ratio} = 0.655) P=m˙wnet=15×127.3=1910 kWP = \dot m w_{net} = 15 \times 127.3 = 1910\ \text{kW}

Answer: T2=528.7T_2 = 528.7 K; T4=751.4T_4 = 751.4 K; wnet=127.3w_{net} = 127.3 kJ/kg; ηth=20.4%\eta_{th} = 20.4\%; work ratio = 0.345; P=1910P = 1910 kW.

✓ Answer checked by Claude Opus 5.5 (high effort)

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