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Computational and Experimental
Investigation of
Aerodynamics of Flapping Airfoils
Group members
K.M.G.L. Dilshan
D.H.S. Abenayake
W.M.K.S. Weerasekara
M.L.L.U. Gunaratne
1
2
Real bird Simplified model
Flapping Motion
3
Aim
• To develop a computational and experimental framework to
investigate the aerodynamic characteristics of flapping airfoils
Objectives
• To develop a computational framework to capture flapping wing
motion and flow characteristics
• To design and develop an experimental setup with a data acquisition
system to obtain flow properties
• Analyze how the propulsion effect can be improved with varying
flapping characteristics
4
Computational Framework
• Inviscid flow model
• Viscous flow model
Experimental Framework
• Flow visualisation setup
• Force calculation setup
Project
methodology
5
Validation of the viscous model
Experimental ClXFOIL ClANSYS Cl
ANSYS Cd XFOIL Cd
6
• K-ω Shear Stress Transfer RANS model was chosen
Validation of the viscous model
7
Validation of the viscous model
Experimental Cl
Simulated Cl
Cp Experimental Cp
Simulated
• Number of elements was varied from 15,000 to 980,000
8
Final Mesh
Final Mesh
• Average skewness 0.21
• Average orthogonal quality
0.925
• Number of Elements 484,000
Mesh input parameters
• Angle of attack
• Distance from the front
of the airfoil
• Distance from the back of
the airfoil
Velocity field variation in plunging at 5Hz Velocity field variation in pitching at 4Hz
Vorticity field in plunging at 5Hz
User Defined Function parameters
• Plunging frequency
• Plunging amplitude
A combined motion of pitching and
plunging was also developed
10
5Hz Plunging comparison of Cl of 0.05s and 0.02s step sizes
• Considering the simulation time and the gained improvement, along with the range of
variation , the step size of 0.005s was finalized
Time Convergence
11
Inviscid Model Development
12
Inviscid Model Development
Vortex emerging point selection Complete inviscid model
13
Inviscid Model - Validation
14
Inviscid Model - Validation
15
Inviscid Model – Plunging motion
(Frequency: 1Hz, Amplitude: 0.25m, AoA: 0°)
16
Load Cell Design and Manufacturing For Wind Tunnel Testing
• Drag force 0 – 2 N
• Lift force 0 – 4N
• Crosstalk - less than 1%
• Strain required > 10^(-4)
17
Final Design
Lift
Drag
Load Cell
Structur
e
Force Direction Strain X direction Strain Y direction
Lift 3.658 x 10-4 7.172 x 10-7
Drag 1.6719 x 10-6 1.6231 x 10-4
Force Direction Crosstalk X Crosstalk Y
Lift - 0.19%
Drag 0.97% -
18
Manufacturing and Testing
19
Smoke Flow Visualization Setup – Smoke Generating Machine
Liquid
reservoir
Pump
Thermostat
cut off – 2700C
Glass woolAluminium
metal block
Copper tube
Heating element
Nozzle
20
Smoke Flow Visualization Setup – Smoke Rake
21
Smoke Flow Visualization Setup – Steady State Results
progress
22
Plunging Motion – Scotch Yoke Mechanism
23
Plunging Motion – Results
Comparison – Steady-state – Streamline Pattern
0°
10°
15°
Inviscid model CFD model Flow visualization
25
Comparison of lift
coefficient variation
with angle of attack
Comparison – Steady-state – Coefficient of Lift (Cl)
Comparison – Plunging – Coefficient of Lift (Cl) & Coefficient of Drag (Cd)
Comparison – Plunging – Trailing Edge Vortex Shedding (Wake Pattern)
CFD Model
Inviscid Model
Experimental Model
Limitations
Inviscid Model CFD Model Flow Visualization
Only for low Strouhal number region
for plunging
Time consuming – 8hrs Streamlines are not clear in higher
Reynolds numbers
Need to be improved for pitching - Plunging mechanism have limitations
on maximum amplitude and
maximum frequency
Cannot identify flow separation -
Limitations – Experimental load cell apparatus
Effect of moment on lift measurement Effect of moment on drag measurement
Thank You.!
30

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