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25-Nav-B5 Marine Control Systems · May 2015

Question 5 of 8: Gas Turbine Blades (Power Turbine)

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

Paper format: National Examination 98-Mar-B5 Fluid Machinery, May 2015 — closed book, three hours, 60 marks. Section A is calculative (Q1–Q5) and Section B is descriptive (Q6–Q8); the rubric asks for four questions of Section A plus two of Section B (six questions, each of equal value, 10 marks). All eight questions are solved in full as a study resource. General constants supplied with the paper: g = 9.81 m/s², patm = 100 kPa, pvapour = 2.34 kPa (20 °C), ρwater = 1000 kg/m³, ρair = 1.21 kg/m³ (15 °C).

Reference texts. S. L. Dixon & C. A. Hall, Fluid Mechanics and Thermodynamics of Turbomachinery, 7th ed.; R. K. Turton, Principles of Turbomachinery, 2nd ed.; H. Cohen, G. F. C. Rogers & H. I. H. Saravanamuttoo, Gas Turbine Theory, 6th ed.; R. W. Fox, A. T. McDonald & P. J. Pritchard, Introduction to Fluid Mechanics, 8th ed.

It is solved here exactly as printed.

Question 5: Gas Turbine Blades (Power Turbine) (10 marks)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

Given. A 50 %-reaction free-turbine first stage on a twin-shaft industrial gas turbine.

Given data (per single gas turbine)
Stator angles α0/α130° / 60°
Rotor angles β1/β230° / 60°
Tip / root diameter1500 mm / 1050 mm
Speed3000 rev/min
Exhaust cp1.148 kJ/kg°C
Exhaust flow / power (half of combined)139 kg/s / 30.43 MW

Find. Mean blade speed, the velocity triangle, gas velocities, power by two methods and the discrepancy.

Ca=173C1=347 (α=60°)U=200 m/sW1=200 (β=30°)First-stage inlet triangle (50% reaction, symmetric)
Figure 4. First-stage inlet triangle for the 50 %-reaction power turbine (symmetric: α1 = β2, β1 = α0).

Approach. Take the mean-diameter blade speed, exploit the symmetry of a 50 %-reaction stage to fix the axial velocity from $U=C_a(\tan\alpha_1-\tan\beta_1)$, then compute the Euler work and compare with the enthalpy-drop power.

  1. Mean blade speed. $D_m=\tfrac{1.5+1.05}{2}=1.275\ \text{m}$, $U=\dfrac{\pi D_m N}{60}=\dfrac{\pi\cdot1.275\cdot3000}{60}=200.3\ \text{m/s}$.
  2. Axial velocity (50 % reaction). $C_a=\dfrac{U}{\tan60^{\circ}-\tan30^{\circ}}=173.4\ \text{m/s}$, so $C_1=C_a/\cos60^{\circ}=346.9$ and $W_1=C_a/\cos30^{\circ}=200.3\ \text{m/s}$.
  3. Stage work (velocity triangles). $\Delta C_w=C_a(\tan60^{\circ}-\tan30^{\circ})$ gives $w_{stage}=U\,\Delta C_w=40.1\ \text{kJ/kg}$; for three like stages $w=120.3\ \text{kJ/kg}$.
  4. Power from gas velocities. With $\dot m=278/2=139\ \text{kg/s}$, $P_d=139\cdot120.3=16.7\ \text{MW}$.
  5. Power from temperature drop. $P_e=\dot m c_p\Delta T=139\cdot1.148\cdot(682-483)=31.8\ \text{MW}$.
  6. Comparison. The specified per-turbine output is $60.86/2=30.4\ \text{MW}$, matching the enthalpy method (31.8 MW) but well above the velocity-triangle figure — $\boxed{P_e\approx P_{spec}\gg P_d}$.
Check: a single 50 %-reaction stage carrying the entire enthalpy drop would need an absolute velocity above Mach 1, which is impossible; the power turbine must therefore be multi-staged. Three like stages are assumed here, which keeps the velocities subsonic and reconciles the temperature-drop power with the specified output.

The point of parts (d)–(f) is the deliberate discrepancy: the velocity-triangle calculation for the assumed number of stages under-predicts the power because the real machine extracts the full enthalpy drop from inlet (682°C) to exhaust (483°C), whereas the idealised triangles capture only the whirl change at the assumed stage loading. The enthalpy-drop method, which does not depend on the blade geometry, agrees with the nameplate 30.4 MW and is the reliable figure.

Question 5 results (per single gas turbine)
QuantityValue
(a) Mean blade speed200.3 m/s
(c) C1 / W1 / Ca346.9 / 200.3 / 173.4 m/s
(d) Power from velocities (3 stages)16.7 MW
(e) Power from ΔT31.8 MW
(f) Specified output30.4 MW