Question 3 of 8: Steam Turbine Blades — Velocity Diagram
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper: National Examinations — 07-Mec-A6 Fluid Machinery, May 2013. Closed-book, three hours. Section A (Calculative) Q1–Q5, Section B (Descriptive) Q6–Q8; the candidate answers four from A and two from B, six questions of equal value (10 marks each). All eight questions are worked here as a complete study resource.
Reference texts: R. K. Turton, Principles of Turbomachinery; S. L. Dixon & C. A. Hall, Fluid Mechanics and Thermodynamics of Turbomachinery; R. W. Fox, A. T. McDonald, Introduction to Fluid Mechanics; Douglas, Gasiorek & Swaffield, Fluid Mechanics. Constants as printed on the exam attachment pages (g = 9.81 m/s², patm = 100 kPa, pvapour = 2.34 kPa at 20°C, ρwater = 1000 kg/m³).
Combined velocity diagram (blade velocity V_B as the common base). Inlet triangle in red/blue, outlet in purple/green; the horizontal gap between the absolute tips is the change in whirl.
Approach. Resolve the inlet absolute velocity into whirl and axial components, build the inlet relative velocity, mirror it (with the 0.95 friction factor) through the symmetrical blade, then recombine to get the exit absolute velocity; the change of whirl gives the tangential force, hence power and efficiency.
Inlet relative velocity. $V_{R1}=\sqrt{(V_{w1}-V_B)^2+V_{a1}^2}=\sqrt{172.9^2+153.9^2}=231.5$ m/s at $\beta_1=\tan^{-1}\!\dfrac{153.9}{172.9}=41.7^\circ$.
Outlet relative velocity (friction + symmetry). $V_{R2}=0.95\,V_{R1}=219.9$ m/s at $\beta_2=\beta_1=41.7^\circ$. Its whirl component (opposing the blade) is $V_{R2}\cos\beta_2=164.2$ m/s and axial $V_{R2}\sin\beta_2=146.2$ m/s.
(a) Exit absolute velocity. $V_{w2}=V_B-V_{R2}\cos\beta_2=250-164.2=85.8$ m/s; $V_{a2}=146.2$ m/s. Then $V_{S2}=\sqrt{85.8^2+146.2^2}$, giving $\boxed{V_{S2}=170\ \text{m/s at }\delta=59.6^\circ}$ to the plane of rotation.
(b) Power from change of whirl. $\Delta V_w=V_{w1}-V_{w2}=422.9-85.8=337.1$ m/s; tangential force $F=\dot m\,\Delta V_w=30(337.1)=10.11$ kN; $P=F\,V_B=10.11\times10^{3}(250)$, so $\boxed{P=2.53\ \text{MW}}$.
(c) Blade efficiency. $\eta_b=\dfrac{V_B\,\Delta V_w}{V_{S1}^2/2}=\dfrac{250(337.1)}{450^2/2}$, so $\boxed{\eta_b=83.2\%}$.