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Axial gas turbine stage design calculation

Short answer

Cw2 = 250 tan65° = 536.1 m/s. Rotor inlet β2 = atan((536.1-340)/250) = 38.1°, exit β3 = atan(340/250)=53.7°. Work w = 340×536.1 = 182.3 kJ/kg, ΔT0=158.8 K. Reaction R=1-536.1/680=0.212. Stagnation pressure ratio 1.92, power 4.56 MW.

An axial-flow gas turbine stage has a mean blade speed of 340 m/s and a constant axial velocity of 250 m/s. The nozzle exit angle is 65 degrees and the gas leaves the stage in the axial direction (no exit swirl). The inlet stagnation temperature is 1200 K, the total-to-total stage efficiency is 0.88, cp=1.148c_p = 1.148 kJ/kg K and γ=1.333\gamma = 1.333. Find (a) the rotor blade angles at inlet and outlet, (b) the work per kg and the stagnation temperature drop, (c) the degree of reaction, (d) the stagnation pressure ratio, and (e) the power for a flow of 25 kg/s.

Data: U=340U = 340 m/s, Ca=250C_a = 250 m/s, α2=65∘\alpha_2 = 65^\circ (nozzle exit), α3=0\alpha_3 = 0, T01=1200T_{01} = 1200 K, ηtt=0.88\eta_{tt} = 0.88. Stations: 1 nozzle inlet, 2 nozzle exit/rotor inlet, 3 rotor exit.

 Rotor inlet                 Rotor exit
      C2                         Vr3   C3=Ca
     /|\ Vr2                      \    |
    / | \                          \b3 |
   /65|b2\                          \  |
  +---U---+                       ---U-+

(a) Blade angles

Cw2=Catan⁡65∘=250×2.1445=536.1 m/sC_{w2} = C_a\tan 65^\circ = 250 \times 2.1445 = 536.1\ \text{m/s} tan⁡β2=Cw2−UCa=196.1250⇒β2=38.1∘\tan\beta_2 = \frac{C_{w2} - U}{C_a} = \frac{196.1}{250} \Rightarrow \beta_2 = 38.1^\circ

At exit Cw3=0C_{w3} = 0, so the relative whirl is UU:

tan⁡β3=UCa=340250⇒β3=53.7∘\tan\beta_3 = \frac{U}{C_a} = \frac{340}{250} \Rightarrow \beta_3 = 53.7^\circ

(b) Work and temperature drop

w=U(Cw2+Cw3)=340×536.1=182.3 kJ/kgw = U(C_{w2} + C_{w3}) = 340 \times 536.1 = 182.3\ \text{kJ/kg} ΔT0=wcp=182.31.148=158.8 K\Delta T_0 = \frac{w}{c_p} = \frac{182.3}{1.148} = 158.8\ \text{K}

(c) Degree of reaction

R=Ca2U(tan⁡β3−tan⁡β2)=1−Cw22U=1−536.1680=0.212R = \frac{C_a}{2U}(\tan\beta_3 - \tan\beta_2) = 1 - \frac{C_{w2}}{2U} = 1 - \frac{536.1}{680} = 0.212

(d) Pressure ratio

From ηtt=ΔT0T01(1−(p03/p01)(γ−1)/γ)\eta_{tt} = \dfrac{\Delta T_0}{T_{01}(1 - (p_{03}/p_{01})^{(\gamma-1)/\gamma})}:

p01p03=[1−ΔT0ηttT01]−γ/(γ−1)=[1−158.80.88×1200]−4.003=1.92\frac{p_{01}}{p_{03}} = \left[1 - \frac{\Delta T_0}{\eta_{tt}T_{01}}\right]^{-\gamma/(\gamma-1)} = \left[1 - \frac{158.8}{0.88 \times 1200}\right]^{-4.003} = 1.92

(e) Power

P=m˙w=25×182.3=4557 kW=4.56 MWP = \dot m w = 25 \times 182.3 = 4557\ \text{kW} = 4.56\ \text{MW}

Stage loading w/U2=1.58w/U^2 = 1.58 and flow coefficient Ca/U=0.74C_a/U = 0.74.

Answer: β2=38.1∘\beta_2 = 38.1^\circ, β3=53.7∘\beta_3 = 53.7^\circ; w=182.3w = 182.3 kJ/kg, ΔT0=158.8\Delta T_0 = 158.8 K; R=0.212R = 0.212; p01/p03=1.92p_{01}/p_{03} = 1.92; P=4.56P = 4.56 MW.

✓ Answer checked by Claude Opus 5.5 (high effort)

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