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Impulse stage: blade angles, work and thrust

Short answer

Using velocity triangles with C1=600 m/s, α1=20°, U=250 m/s, k=0.9, symmetrical blades: inlet blade angle β1=33.2°. Exit velocity C2=187.5 m/s at 80.0°. Work w=149.1 kJ/kg gives power 1491 kW. Diagram efficiency 82.8%. Axial thrust 205 N.

In a single-stage impulse turbine the nozzle angle is 20 degrees and the steam leaves the nozzle at 600 m/s. The blade speed is 250 m/s and the blades are symmetrical (equal inlet and outlet angles). The blade velocity coefficient is 0.9. For a steam flow of 10 kg/s, find (a) the blade angles, (b) the absolute velocity and direction at exit, (c) the power developed, (d) the diagram efficiency, and (e) the axial thrust. Neglect axial-velocity change due to friction other than that given by the velocity coefficient.

Data: α1=20∘\alpha_1 = 20^\circ, C1=600C_1 = 600 m/s, U=250U = 250 m/s, k=0.9k = 0.9, m˙=10\dot m = 10 kg/s. Symmetrical blades: β1=β2\beta_1 = \beta_2.

(a) Inlet velocity triangle and blade angles

Cw1=C1cos⁡20∘=563.8 m/s,Ca1=C1sin⁡20∘=205.2 m/sVw1=Cw1−U=313.8 m/sVr1=Vw12+Ca12=375.0 m/s,tan⁡β1=Ca1Vw1⇒β1=33.2∘\begin{aligned} C_{w1} &= C_1\cos 20^\circ = 563.8\ \text{m/s}, \quad C_{a1} = C_1\sin 20^\circ = 205.2\ \text{m/s} \\ V_{w1} &= C_{w1} - U = 313.8\ \text{m/s} \\ V_{r1} &= \sqrt{V_{w1}^2 + C_{a1}^2} = 375.0\ \text{m/s}, \quad \tan\beta_1 = \frac{C_{a1}}{V_{w1}} \Rightarrow \beta_1 = 33.2^\circ \end{aligned}

Blade inlet angle = blade outlet angle = 33.2 degrees.

(b) Outlet velocity triangle

Vr2=kVr1=0.9×375.0=337.5 m/sVw2=Vr2cos⁡β2=282.4 m/s (backward),Ca2=Vr2sin⁡β2=184.7 m/sCw2=Vw2−U=32.4 m/s (backward, opposite to U)\begin{aligned} V_{r2} &= k V_{r1} = 0.9 \times 375.0 = 337.5\ \text{m/s} \\ V_{w2} &= V_{r2}\cos\beta_2 = 282.4\ \text{m/s (backward)}, \quad C_{a2} = V_{r2}\sin\beta_2 = 184.7\ \text{m/s} \\ C_{w2} &= V_{w2} - U = 32.4\ \text{m/s (backward, opposite to } U\text{)} \end{aligned} C2=Cw22+Ca22=187.5 m/sC_2 = \sqrt{C_{w2}^2 + C_{a2}^2} = 187.5\ \text{m/s}

The absolute exit velocity is 187.5 m/s at an angle α2=tan⁡−1(Ca2/∣Cw2∣)=80.0∘\alpha_2 = \tan^{-1}(C_{a2}/|C_{w2}|) = 80.0^\circ to the blade direction.

(c) Power

w=U(Vw1+Vw2)=250×(313.8+282.4)=149.1 kJ/kgw = U(V_{w1} + V_{w2}) = 250 \times (313.8 + 282.4) = 149.1\ \text{kJ/kg} P=m˙w=10×149.1=1491 kWP = \dot m w = 10 \times 149.1 = 1491\ \text{kW}

(d) Diagram efficiency

ηd=wC12/2=149.1180.0=0.828\eta_d = \frac{w}{C_1^2/2} = \frac{149.1}{180.0} = 0.828

(e) Axial thrust

Fa=m˙(Ca1−Ca2)=10×(205.2−184.7)=205 NF_a = \dot m (C_{a1} - C_{a2}) = 10 \times (205.2 - 184.7) = 205\ \text{N}

Answer: blade angles 33.2∘33.2^\circ; exit velocity 187.5 m/s at 80.0∘80.0^\circ; power 1491 kW; ηd\eta_d = 82.8%; axial thrust 205 N.

✓ Answer checked by Claude Opus 5.5 (high effort)

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