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04-BS-7 · December 2019

Question 6 of 13: Thrust Developed by an Aircraft Propeller

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

Notes on this paper

04-BS-7 Mechanics of Fluids — December 2019 (National Examinations, three hours, closed book). Section A (Calculative) offers 9 questions and instructs “do seven”; Section B (Analytical) offers 4 questions and instructs “do three.” Every question is answered below (13 of 13), so students can use the full paper as a study resource. Constants used throughout (from the paper's own Constants page): g = 9.81 m/s², patm = 100 kPa, ρwater = 1000 kg/m³, SGglycerine = 1.26, SGmercury = 13.56, ρconcrete = 2400 kg/m³, ρair = 1.19 kg/m³ (20°C) / 1.21 kg/m³ (15°C), μwater = 1.0×10⁻³ N·s/m², μair = 1.8×10⁻⁵ N·s/m², Rair = 287 J/kg·K.

Reference texts: F. M. White, Fluid Mechanics, 8th ed. (McGraw-Hill) — fluid statics and manometry (Ch. 2), hydrostatic forces and the middle-third rule (Ch. 2), buoyancy and equilibrium (Ch. 2), dimensional analysis and drag (Ch. 5, 7), pipe friction and the Moody/Colebrook relation (Ch. 6), control-volume momentum and propeller/actuator-disk theory (Ch. 3, 11); J. D. Anderson, Fundamentals of Aerodynamics — wave/compressibility drag divergence (Ch. 5) for the Boeing 747 wind-tunnel chart used in Question 9.

Question 6: Thrust Developed by an Aircraft Propeller (5 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.

The value is consistent with a large propeller aircraft cruise speed well below the 650 km/hr slipstream exit speed the question also gives.

Given.

QuantityValue
Propeller diameter, D2 m
Aircraft (upstream) velocity, V1500 km/hr
Slipstream exit velocity, V2650 km/hr
Air density (Constants, p.12, 15°C)1.21 kg/m³
V1=500 km/hr V2=650 km/hr
Actuator-disk model: streamtube converges through the propeller as velocity rises from V1 to V2; thrust equals the momentum change of the mass flow through the disk.

Find. The thrust developed by the propeller.

Approach. Model the propeller as an actuator disk: the mass flow rate through the disk uses the AVERAGE of the far-upstream and far-downstream velocities (since the streamtube converges and the velocity at the disk itself is the mean of the two), and thrust is that mass flow rate times the overall velocity change.

  1. Convert velocities and find the disk (mean) velocity. $$V_1=500\times\frac{1000}{3600}=138.9\ \text{m/s}\qquad V_2=650\times\frac{1000}{3600}=180.6\ \text{m/s}$$ $$V_{disk}=\frac{V_1+V_2}{2}=\boxed{159.7\ \text{m/s}}$$
  2. Mass flow rate through the disk. $$A=\frac{\pi}{4}D^2=\frac{\pi}{4}(2)^2=3.1416\ \text{m}^2$$ $$\dot{m}=\rho A V_{disk}=(1.21)(3.1416)(159.7)=\boxed{607.2\ \text{kg/s}}$$
  3. Thrust from the momentum change. $$F_{thrust}=\dot{m}(V_2-V_1)=(607.2)(180.6-138.9)=(607.2)(41.67)$$ $$\boxed{F_{thrust}=25.30\ \text{kN}}$$
QuantityValue
V1 / V2138.9 / 180.6 m/s
Disk (mean) velocity159.7 m/s
Mass flow rate607.2 kg/s
Thrust25.30 kN