end of semester project summary for the morphing wing ...mason/mason_f/morphf04pres.pdf · 0.8 1...
TRANSCRIPT
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End of Semester Project Summary for the Morphing Wing Design Team
Desta AlemayehuMathieu LengRyan McNulty Michael MulloyRyan SomeroCyril de Tenorio
December 13, 20041
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Request for Proposal (RFP) from the Center for Intelligent Materials Systems and Structures
Design and build a morphing wing aircraft which can operate in four configurations
The four configurations are Dash,Maneuver, Loiter, and Landing
Similar to the aircraft currently beingdeveloped by NextGen.
Four configurations from NextGen design [NextGen, 2004]
December 13, 20042
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The work presented identifies the process used to design, build and test a morphing wing
Results and conclusions
Full scale wing model
Airfoil shape models
December 13, 20043
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Three important factors drove the design and construction of the wing
Feasibility 1. Weight2. Actuation / structural arrangement3. Aerodynamics4. Structures 5. Flight Controls
Time1. Design2. Constructions3. Testing
Cost ($5,000 budget )
Due to time constraints alternative methods of morphing were not considered.
December 13, 20044
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The following are the project goals for the year
Fall 2004
1. Design the morphing wing and build semi-span of the wing for testing in the wind tunnel.
2. Show that the wing can morph under aerodynamic load
3. Prove the concept is feasible for implementation on a model airplane
Spring 2005
1. Implement the morphing wing design on a model airplane
2. Conduct flight testing to validate design
December 13, 20045
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The total estimated weight for the aircraft was 13.97 lbs.
The initial weight estimation was done by categorizing the parts needed for construction into five components
The weight for each part was acquired from the manufacturer
COMPONENT WEIGHT
Propulsion Weight 3.65 lbs
Landing Gear Weight 1.41 lbs
Wing Weight 3.40 lbs
Fuselage and Tail Weight 3.26 lbs
Payload Weight 2.25 lbs
Total Weight 13.97 lbs
December 13, 20046
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Total weight for the model airplane should be close to 10 -11 lbs.
The weight estimate was compared to existing model air planes
December 13, 20047
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Three initial structural and actuation concepts were designed
Rotating Beam Sliding Ribs
C-Socket
December 13, 20048
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After the pros and cons were compared, the C-Socket design was selected
Rotating Beams Sliding Ribs C-Socket
Advantages Limitations Advantages Limitations Advantages Limitations
1) No mechanism inside the wing for actuation
2) Limited need of storage inside fuselage for sweep back
1) Difficulties to implement span change
2) Apparent complexity and time limitation for development
1) Guidance of the trailing ½wing as it is moving, due to the sliding ribs support
2) Twist resistance at the level of the ribs
1) The beams have to be placed too close from the edges
2) Lack of confidence in the pin to support the loads due to twist
3) Holes in the wing in the deployed position
1) Possibility to place the main spar at ¼ chord
2) Available space at mid-chord.
3) Span, Chord, and sweep changes can be implemented with this design
1) Twist only supported by the screw mechanism
December 13, 20049
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Sweep actuation consists of a motor driven power screw
An electric motor drives apower screw
A transverse nut travels up the screw length
Push rods retract and increase sweep
December 13, 200410
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Chord change actuation consists of chain driven power screws
An electric motor drives a chainsprocket system
The sprockets are mounted onpower screws
The screws expand or retractthe two main wing spars
December 13, 200411
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December 13, 200412
Span change is actuated by a sail winch servo
The main spar houses a smaller diameter extension spar
A winch servo is counter wrapped with 50 lb test fishing line
As the servo turns, one line unwraps while the other pulls the extension in or out
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Sweep and chord changes are controlled by electric motors in a polarity changing circuit
The circuits are each powered by a 9 V battery
When the wing morph reachesa max a kill switch is tripped
The toggle switch controls thepolarity and engages the motor
The potentiometer acts as a speed controller by varying the motor voltage
December 13, 200413
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Implementing all three actuators in the wing produces our final model
December 13, 200414
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Since the wind tunnel cross-section is 6’x6’ we were unable to use the instrumentation strut
The testing strut is over 3’ tall
The full size wing is 4’-4”
To avoid wall effects we had to allow a 1’ clearance
Building our own strut wastoo time consuming
December 13, 200415
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The Clark Y was chosen because the flat bottom simplifies the construction and chord change
Because time constraints the airfoil selection for the wing was based only on the requirements of the actuation and not the aerodynamic performance need for optimal performance in the four configurations.
December 13, 200416
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To simplify the construction the full scale wing was built in three different components.
December 13, 200417
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The potential for flow separation with the chord extended was a reason for wind tunnel testing
Cp
x/c
The pressure coefficient crossing the axis shows the potential for separation at the location of the chord extension
December 13, 200418
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The Selig 8036 and the Eppler 168 were chosen to challenge the Clark Y
The Selig 8036 was chosen due to its high estimated maximum Cl and controlled stall0
0.2
0.4
0.6
0.8
1
1.2
1.4
0 5 10 15 20 25
Angle of Attack ( Degrees)
The extended Clark Y estimated aerodynamic performance was used as the baseline for comparison
December 13, 200419
0
0.2
0.4
0.6
0.8
1
1.2
1.4
0 5 10 15 20 25
Angle of Attack (Degrees)
Cl
Cd
Cl
Cd
The Eppler 168 was chosen because it showed potential for lower drag and a later stall than the Clark Y
0
0.2
0.4
0.6
0.8
1
1.2
0 5 10 15 20 25
Angle of Attack ( Degrees)
Cl
Cd
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The wind tunnel models were constructed from spider foam and carbon fiber
The foam cores were ordered from FlyingFoam.com Bi-directional Carbon Fiber was
epoxyed to the foam cores.
December 13, 200420
The models were finally sanded for smoothness.
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Tests in the wind tunnel were needed to validate the wing design
Some questions concerning the chord extension could not be answered using theory :
Separation?
Aerodynamic benefit from extension?
December 13, 200421
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Apparatus and instrumentation used for testing of the foam wing models
Virginia Tech Stability Wind Tunnel• Test section: 24 feet long, 6x6 feet in cross-section• Max speed: 275 ft/s
6 Wind Tunnel Models• 4 feet in span and 0.64 feet in chord: this choice was made to match the Aspect Ratio of the morphing wing• Airfoils: original and extended-chord version of the Clark-Y, Selig 8036, and Eppler168
Stability Tunnel Strut Mount• Located in the middle of the test section• Equipped with a six-component strain gauge balance and an automated angle of attack-sweep system
December 13, 200422
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The following is important test information
A total of 24 runs were performed:• Longitudinal tests (-6 to 20deg alpha-sweep)• Flow visualization
The choice of the tunnel speeds was made to match the Reynolds number of the morphing aircraft in actual flight conditions
Flow visualization was achieved using 1.5” long yarn tufts arranged in three rows on the upper surface of the model
December 13, 200423
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December 13, 200424
The following strategy was applied to test the foam models
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The flow separation on the extended models was acceptable
No early separation was observed on critical parts of the extended
wing
Progressive stall behavior allowing pilot correction before stall
Progressive evolution
Steady growth of CL
Free stream
Stabilization of separation
No change in CL
Separation “pop”
αmax αpopα0L
CL
α
December 13, 200425α0L αpopαmax
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December 13, 200426
By comparing the lifting performance of the different models, the Clark Y is the best choice
CL*
-0.6
-0.4
-0.2
0
0.2
0.4
0.6
0.8
1
1.2
1.4
-10 -5 0 5 10 15 20 25
Clark Y - e
Clark Y - r
Eppler - r
Eppler - e
Selig - r
Selig - e
α
[º]
CL*
r ≡ retracted
e ≡ extended
mincbqL××
≡
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December 13, 200427
By comparing the lifting performance of the different models, the Clark Y is the best choice.
-0.6
-0.4
-0.2
0
0.2
0.4
0.6
0.8
1
1.2
1.4
-5 0 5 10 15 20 25
Clark Y - e
Clark Y - r
Eppler - r
Eppler - eSelig - r
Selig - e
CL*
α∗
[º] L0* ααα −≡Note:
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Reviewing different aerodynamic characteristics confirms the choice of the Clark Y
0
0.02
0.04
0.06
0.08
0.1
0.12
r e r e r e
CLARK Y Selig Eppler
CLα[/deg]
December 13, 200428
0246
8101214
r e r e r e
CLARK Y Selig Eppler
a*Max[deg]
0
0.2
0.4
0.6
0.8
1
1.2
r e r e r e
CLARK Y Selig Eppler
CLmax
With a high CLα and a long α−range, the Clark Y can reach the highest value in lift.
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December 13, 200429
Clark Y performance results from wind tunnel testing
CLARK Y
CL = 0.1021α∗
CL= 0.0678α∗
-0.4
-0.2
0
0.2
0.4
0.6
0.8
1
1.2
1.4
-5 0 5 10 15 20 25
alpha*
CL
Stall for retracted
Stall for extendedCLmax=1.19
α *max=12 deg
α 0L=-6 deg
CLmax=0.92
α *max=14 deg
α 0L=-4 deg
Extended
Retracted
α∗
[º]
CL*
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The following are conclusions based on the wind tunnel testing of the foam models
Flow visualization showed that the extended-ClarkY doesnot stall as predicted.
The chord extension mechanism improves the liftingCharacteristics.
The aerodynamic performances between the Clark-Y, Selig8036 and Epler168 airfoils reaffirms our original design choice of using the Clark-Y.
December 13, 200430
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The following are conclusions based on the wind tunnel testing of the foam models
Critical aerodynamic data were obtained for the retracted and extended configuration of the Clark-Y:
– CLmax = 1.19– CLα = 0.1021/º extended & 0.0678 /º retracted
Based on these results we can deduce a take off velocity of 30 Mph assuming a lift off CL* of 1.1 (which correspond to CL=0.8 and a = 6º).
Note: the surface roughness of the model might have been a factor concerning the separation pattern
December 13, 200431
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The image below shows the wind tunnel setup used for the full scale wing
Flow directions
Positive Angle of attack
Span Change
Chord Change
Four rows of tuft ~2 in long Tuft on
attachment system
December 13, 200432
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December 13, 200433
Test velocity = 30 -35 mph (Takeoff speeds)Angle of attack range = 0 – 25 degrees
Test case 1:Flow visualization for NO span and NO chord change, normal wing.Determine approximate stall angel of attack
Test Case 2:Span change under aerodynamic loads and flow visualizations Determine approximate stall angle of attack
Test case 3:Flow visualization for Chord change Determine Approximate stall angle of attack
Test Case 4:Flow visualization for span and chord change Determine approximate stall angle of attack
Special Case:Look at flow interaction between Mounting system and wing
Proposed setup for the full scale wing wind tunnel tests
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Test Conditions
Date: Thursday 11/18/04 4:45 AMTunnel Temperature: 64.6 o FOutside Temperature: 52 o FPressure: 28.01 ins of Hg
Actual Test Matrix
Case one: NO span and NO chord
Increased angle of attack at a velocity ~ 20 mph. Considerable motion of the wing TEST ABORTED.
Increase angle of attack to 10 degrees with tunnel at ideal and increased velocity. Considerable motion of the wing at ~25 mph TEST ABORTED
The per-test matrix was not used during wing tunnel tests because of safety concerns.
December 13, 200434
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In conclusion, next semester we hope to build and fly a fully functional radio controlled model
Design control surfaces and their actuation
Moving mass to counter center of gravity from wing sweep
Focus on two major dimension changes instead of three minor changes
Design, build and fly a morphing radio controlled aircraft Questions?
December 13, 200435