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Aeroelastic Behavior of a Typical Airfoil Section
with Shape Memory Alloy Springs
Vagner Candido de Sousa*
Department of Aeronautical Engineering
Engineering School of Sao Carlos
University of Sao Paulo, Brazil
* Visiting Scholar at the Dynamic and Smart Systems Lab
The University of Toledo (Summer/Fall, 2015)
Where we are
2
São Carlos
Campus
Research center
São Paulo
(Capital)
State of São Paulo
São Carlos - SP
Brazil
University of São Paulo
• A state university founded in 1934
• Campi: São Paulo (4), Bauru,
Piracicaba, Pirassununga, Lorena,
Ribeirão Preto, São Carlos (2)
• Undergrads: 58.204
• MSc: 14.149, PhD: 15.398
• Other: 5.041
• Professors: 6.008
• Articles: 16.013 (WoS/ISI)
3
* 2013
Campus 1
University of São Paulo, Campus of São Carlos
• Institute of Physics
• Institute of Mathematic and
Computer Sciences
• Institute of Architecture
• Institute of Chemistry
• Engineering School of São Carlos
– Dep. of Aeronautical Eng.
– Dep. Electrical Eng.
– Dep. Geotechnical Eng.
– Dep. Hydraulics
– Dep. Materials Eng.
– Dep. Mechanical Eng.
– Dep. Production Eng.
– Dep. Structural Eng.
– Dep. Transportation Eng.
4
Department of Aeronautical Engineering
• Research
– Aerodynamics
– Aeroservoelasticity
– Flight Dynamics
– Aeronautical Structures
5
Our lab – Laboratory of Aeroelasticity
6
• Students (Summer, 2015)
– MSc: 1
– PhD: 6
– Post doc: 1
• Collaborations in
– USA
– Canada
– UK
• Facilities
– Blower wind tunnel
– Whirl Tower
– Smart table
– Sensors (accelerometers, laser
vibrometer)
– Acquisition system (dSPACE, LMS Scadas,
LDS Photon)
– Shakers (Modal Shop, APS Long-Stroke
Vibration Exciter)
Current topics of interest
• Fixed-wing and rotary-wing
aeroelasticity
• Smart materials for energy
harvesting and/or vibration control
• Wind energy harvesting (fixed and
rotary wing )
• Shape memory alloys
• Helicopters vibration damping
(piezoelectric based pitch link
device)
• Self-powered circuits for
piezoelectric active/semi-
active/semi-passive control
• Bio-inspired aircraft (morphing) and
aquatic robots
• In short,
Aeroelasticity
+
smart materials
7
Aeroelasticity
• Interaction between
aerodynamic forces and
structural motions
• Airfoil and non-airfoil structures
• Transmission lines
• Suspension bridges
• Tall chimneys and
buildings
• Static phenomena
– Divergence
– Control reversal
• Dynamic phenomena
– Buffeting
– Flutter (many kinds)
8
flowsol.co.uk
Wings
Very brief history (incidents related to aeroelasticity)
• 1903 (Prof. Samuel P.) Langley
Monoplane
– Low torsional stiffness wings
• 1916 Handley Page 0/400
Bomber
– Horizontal tail problems
9
Very brief history
• 1918 Fokker D-VIII
– Wing failures in high-speed
dives
• 1925 Albatros D.III
– Lower wing failures
10
Very brief history
• 1930 Junker F-13
– Horizontal tail problems
• Region of strong rising gust in
England
• 1938 Junkers 90-V1
– Crashed during a “non-
conservative” flight test
11
Very brief history
• 1940 Tacoma Narrows Bridge
• Structural failure
• 1959/1960 Lockheed Electra
• In-flight wing break-up
12
Very brief history
• 1960-1970 Rockets
– Problems observed during wind
tunnel tests and corrected
• 1970-1980 Space shuttle
13
An important observation
• Most of those structures had
sufficient strength in static tests
• Problems appeared under
aerodynamic loads
– Related to aeroelastic
phenomena
14
Static aeroelasticity phenomena (elastic + aerodynamic forces)
• Divergence
– Static aerodynamic forces
become too large for the wing
torsional stiffness to resist
– Aerodynamic loads increase the
incidence; increasing incidence
the aerodynamic loads increase
• Wing twists until it breaks
15
Langley’s Aerodrome, 1903
First report of static divergence
Static aeroelasticity (elastic + aerodynamic forces)
• Control reversal
– Wings deform in such a way the
control surfaces do not respond
as expected to the pilot’s
commands
– MiG-25’s (formerly Ye-155R/P)
first flight revealed insufficient
wing rigidity
• The resulting control reversal
was dangerous, and
maneuverability limitations
were imposed
16
– On October 30, 1967
• Aileron reversal caused by
exceeding the instrument
speed limit crashed an Ye-
155P1
Dynamic aeroelasticity (inertial + elastic + aerodynamic forces)
• Buffeting • Flutter (many kinds)
– Coupled bending/torsion
modes
• Airfoil
• Non-airfoil (eg, bridges)
– Galloping
– Stall flutter
– “Whirl mode”
– Potentially catastrophic
17
Dynamic aeroelasticity: buffeting
• Airfoil and non-airfoil structures
• Random vibration
• Usually just inconvenient
18
Laminar flow
Turbulent flow
(vortex shedding)
Flow separation
(transition region)
Surface subject
to turbulent flow
Dynamic aeroelasticity: “galloping” flutter
• Large amplitude, low frequency
oscillation
• Bluff bodies (usually non-airfoil)
– Transmission lines (mostly with
ice accretion)
– Cable affected by vortex
shedding of another cable
19
Dynamic aeroelasticity: stall flutter
• Airfoil and non-airfoil
structures
• Periodic (partial or complete)
flow separation from the
airfoil during the oscillation
• Nonlinear aerodynamic
reaction to the motion of the
structure
– Suspension bridges
– Helicopter rotors (rotorcraft
blades)
– Turbomachinery blades
• Free vortices are generated in the
vicinity of the separation points
• The periodic vortex shedding
creates regions of reduced and
even reversed velocity in the
vicinity of the airfoil
20
Dynamic aeroelasticity: “whirl mode” flutter
• Two Lockheed L-188 “Electra”,
– Braniff Flight 542
• September 29, 1959
• near Buffalo, TX
• 34 fatalities
– NW Orient Airlines Flight 710
• March 17, 1960
• near Cannelton, IN
• 63 fatalities
• disintegrated during flight
– wing brake-up
21
Actual aircraft before crash (stinsonflyer.com)
• In both cases,
– No survivors
– Inconclusive investigations
“Whirl mode” flutter (a new investigation at NASA Langley)
• Wind tunnel tests of an Electra 1/8-
scale model showed:
– Overly stiff wing
– Outboard nacelles responding
differently than intended
– Flutter “passes on” from nacelle to
(even a “flutter-free”) wing
• Growing flutter magnitude
decreased the oscillation
frequency from 5 to 3 Hz
• Wing frequency was also 3 Hz
– Harmonic coupling
22
YouTube channel: NASA Langley CRGIS
Flutter Tests of the Full Span Lockheed Electra
Dynamic aeroelasticity: “whirl mode” flutter (a new investigation)
23
• According to the crash report,
Dynamic aeroelasticity: (aeroelastic) flutter
• Bending/torsion coupled motion
• Self-sustained unstable motion
• Antonov An-148
– March 5, 2011 (test flight)
– near Garbuzovo (350 mi south
of Moscow), Russia
• Airspeed indicator failed
(showing lower airspeed)
• Pilots accelerated 70 mi/h
above the design limit speed
• Low-frequency vibrations
created
• In-flight wing break-up
24
Dynamic aeroelasticity: non-airfoil flutter
• Bending/torsion coupled motion
• Self-sustained unstable motion
• Tacoma Narrows Bridge
– Opened to traffic on July 1, 1940
– Collapsed on November 7, 1940
– Stationary wind design limit: 160 km/h
– Wind speed before failure: 60 km/h
25
Aeroelastic flutter
• Under airflow excitation, structures
may exhibit aeroelastic oscillations
– due to interactions of
aerodynamic, elastic and inertial
forces
• At a critical airflow speed, lifting
surfaces undergo self-sustained
oscillations (linear flutter speed)
– Flutter: bending/torsion coupled
motion with growing amplitudes
• Potentially catastrophic
26
Aeroelastic and vibration control
• Allows flight vehicles to operate
beyond the traditional flutter
boundaries
• Improves ride qualities
• Minimizes vibration fatigue
damage
27
(Giurgiutiu 2000, JIMSS v. 11; Nitzsche et al 2015, JIMSS)
Controlled
Uncontrolled
Grows until the
structure fails
Conventional passive aeroelastic control / flutter prevention
• There is no universal solution
• Frequent strategies
– add mass or redistribute mass
(‘mass balance’)
– increase torsional stiffness, i.e.,
increase ωα
– increase (or decrease) ωh/ωα if it
is near one (for fixed ωα)
– add damping to the structure
(hydraulic dampers)
– require the aircraft to be flown
below its critical Mach number
• Penalties
– Extra weight
– Non-optimized operation
28
(Dowell et al. 2015, A Modern Course in Aeroelasticity, p. 118)
Conventional active aeroelastic control
• Aerodynamic control surfaces
operated by servo-hydraulic
actuators
• Penalties/limitations
– Multiple energy conversions
(mechanical, hydraulic, electrical)
– Large number of parts
• Potential failure sites
• Extra weight
– High vulnerability of the hydraulic
pipes network
– Limited frequency bandwidth
29
(Giurgiutiu 2000, JIMSS v. 11)
Smart materials as an alternative (e.g., piezo actuators)
• Direct conversion of electrical
energy to high-frequency linear
motion (mechanical energy)
• Electrical energy is easier to
transmit throughout the aircraft
(electric lines are much less
vulnerable than hydraulic pipes)
30
(Giurgiutiu 2000, JIMSS v. 11)
(reverse piezoelectric effect)
An example
31
• Active control flap for noise and
vibration reduction
• Piezo-stack actuators
(Straub and King 1996)
Smart materials (piezos)
• Advantages
– Can be embedded in the
structure (e.g. on-blade
actuation)
– High energy/mass ratio
– Direct piezoelectric effect can
also be exploited
• Passive and active strategies
• Sensing and actuation
• Energy harvesting
• Disadvantages
– Piezos (reverse effect)
• Very small strokes (e.g. 0.1%)
• Requires displacement
amplification mechanisms
32
Fixed wing aircraft studies
• Heeg 1993 (NASA Langley)
– Piezoelectric actuators
– Flutter suppression of a rigid
wing supported by springs
– +20% flutter speed
• McGowan et al. 1998
– 12% decrease flutter dynamic
pressure
– 75% decrease gust bending
moment
33
A rotating-wing application of smart materials
• Feszty and Nitzsche 2011
– Carleton University, Canada
• Stiffness modulation using
piezoelectric actuators for vibration
control in helicopters
34
(flight tested)
Nitzsche et al
2015, JIMSS
Flutter can be exploited for wind energy harvesting
• Vibrations in a general sense
can be exploited for energy
harvesting
– Direct piezoelectric effect
• Flutter oscillations can provide a
useful additional source of small
amounts of electrical power
– e.g., for embedded Structural
Health Monitoring systems
– Airfoil-based generators
35
An example
• The RC glider was modified to
include:
– two piezoelectric patches
placed at the roots of the wings
• to harvest energy from wing
vibrations
– a cantilevered piezoelectric
beam installed in the fuselage
• to harvest energy from rigid
body motions of the aircraft
36
(SR Anton and DJ Inman, 2008)
An airfoil model for flutter investigations
37
(Mozaffari-Jovin et al 2015, JVC)
2D problem
How we investigate flutter in our lab
38
• 2-DOF (or 3-DOF)
– Plunge (h)
– Pitch (α)
– (Control surface position, β)
• U∞ is the airflow speed
Experimental 2-DOF airfoil model
39
Pitch DOF
wire springPlunge DOF
springs (2/4)
Numerical results and experimental tests
• Linear case, U = 12 m/s • Nonlinear case (freeplay in the
pitch DOF), U = 10 m/s
40
Continuous lines: experimental, dashed lines: simulation
Linear: Erturk et al. (2010), Appl. Phys. Lett. 96(18)
Nonlinear: Sousa et al. (2011), Smart Mater. Struct. 20(9)
Possibilities of study for an smart airfoil/flutter model
• Aeroelastic control
– Classical aeroelasticity
• Structural reinforcement
• Mass tuning
– “Smart” materials
• Sensing and actuation
– Piezoelectric materials
– Shape memory materials
• Energy Harvesting
• Aeroelastic control + Energy
Harvesting
• Smart materials
• Piezoceramics
(electromechanical coupling)
– Active control (actuation)
– Passive (shunt damping)
– Hybrid
– Energy Harvesting
• SMAs
– Passive control (high loss factor,
hysteretic damping)
– Active control (stiffness and
frequency variation)
41
SMA elements can be included in the airfoil model
(my current work)
42
k
• Motivation:
– Modify the aeroelastic
behavior of the airfoil by
exploiting the pseudoelastic
hysteresis of SMAs
SMA
behavior
Preliminary results: aeroelastic behavior with SMA springs
43
An intermediate case is presented,
44
 1
0 3 N e 11.6 m·sf U 
 
Thank you!
45
Special thanks to:
The University of Toledo and MIME Department, Toledo – OH/USA
Dynamic and Smart Systems Lab (smartsys.eng.utoledo.edu)

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UT2015_GradSem_linkedin

  • 1. Aeroelastic Behavior of a Typical Airfoil Section with Shape Memory Alloy Springs Vagner Candido de Sousa* Department of Aeronautical Engineering Engineering School of Sao Carlos University of Sao Paulo, Brazil * Visiting Scholar at the Dynamic and Smart Systems Lab The University of Toledo (Summer/Fall, 2015)
  • 2. Where we are 2 São Carlos Campus Research center São Paulo (Capital) State of São Paulo São Carlos - SP Brazil
  • 3. University of São Paulo • A state university founded in 1934 • Campi: São Paulo (4), Bauru, Piracicaba, Pirassununga, Lorena, Ribeirão Preto, São Carlos (2) • Undergrads: 58.204 • MSc: 14.149, PhD: 15.398 • Other: 5.041 • Professors: 6.008 • Articles: 16.013 (WoS/ISI) 3 * 2013 Campus 1
  • 4. University of São Paulo, Campus of São Carlos • Institute of Physics • Institute of Mathematic and Computer Sciences • Institute of Architecture • Institute of Chemistry • Engineering School of São Carlos – Dep. of Aeronautical Eng. – Dep. Electrical Eng. – Dep. Geotechnical Eng. – Dep. Hydraulics – Dep. Materials Eng. – Dep. Mechanical Eng. – Dep. Production Eng. – Dep. Structural Eng. – Dep. Transportation Eng. 4
  • 5. Department of Aeronautical Engineering • Research – Aerodynamics – Aeroservoelasticity – Flight Dynamics – Aeronautical Structures 5
  • 6. Our lab – Laboratory of Aeroelasticity 6 • Students (Summer, 2015) – MSc: 1 – PhD: 6 – Post doc: 1 • Collaborations in – USA – Canada – UK • Facilities – Blower wind tunnel – Whirl Tower – Smart table – Sensors (accelerometers, laser vibrometer) – Acquisition system (dSPACE, LMS Scadas, LDS Photon) – Shakers (Modal Shop, APS Long-Stroke Vibration Exciter)
  • 7. Current topics of interest • Fixed-wing and rotary-wing aeroelasticity • Smart materials for energy harvesting and/or vibration control • Wind energy harvesting (fixed and rotary wing ) • Shape memory alloys • Helicopters vibration damping (piezoelectric based pitch link device) • Self-powered circuits for piezoelectric active/semi- active/semi-passive control • Bio-inspired aircraft (morphing) and aquatic robots • In short, Aeroelasticity + smart materials 7
  • 8. Aeroelasticity • Interaction between aerodynamic forces and structural motions • Airfoil and non-airfoil structures • Transmission lines • Suspension bridges • Tall chimneys and buildings • Static phenomena – Divergence – Control reversal • Dynamic phenomena – Buffeting – Flutter (many kinds) 8 flowsol.co.uk Wings
  • 9. Very brief history (incidents related to aeroelasticity) • 1903 (Prof. Samuel P.) Langley Monoplane – Low torsional stiffness wings • 1916 Handley Page 0/400 Bomber – Horizontal tail problems 9
  • 10. Very brief history • 1918 Fokker D-VIII – Wing failures in high-speed dives • 1925 Albatros D.III – Lower wing failures 10
  • 11. Very brief history • 1930 Junker F-13 – Horizontal tail problems • Region of strong rising gust in England • 1938 Junkers 90-V1 – Crashed during a “non- conservative” flight test 11
  • 12. Very brief history • 1940 Tacoma Narrows Bridge • Structural failure • 1959/1960 Lockheed Electra • In-flight wing break-up 12
  • 13. Very brief history • 1960-1970 Rockets – Problems observed during wind tunnel tests and corrected • 1970-1980 Space shuttle 13
  • 14. An important observation • Most of those structures had sufficient strength in static tests • Problems appeared under aerodynamic loads – Related to aeroelastic phenomena 14
  • 15. Static aeroelasticity phenomena (elastic + aerodynamic forces) • Divergence – Static aerodynamic forces become too large for the wing torsional stiffness to resist – Aerodynamic loads increase the incidence; increasing incidence the aerodynamic loads increase • Wing twists until it breaks 15 Langley’s Aerodrome, 1903 First report of static divergence
  • 16. Static aeroelasticity (elastic + aerodynamic forces) • Control reversal – Wings deform in such a way the control surfaces do not respond as expected to the pilot’s commands – MiG-25’s (formerly Ye-155R/P) first flight revealed insufficient wing rigidity • The resulting control reversal was dangerous, and maneuverability limitations were imposed 16 – On October 30, 1967 • Aileron reversal caused by exceeding the instrument speed limit crashed an Ye- 155P1
  • 17. Dynamic aeroelasticity (inertial + elastic + aerodynamic forces) • Buffeting • Flutter (many kinds) – Coupled bending/torsion modes • Airfoil • Non-airfoil (eg, bridges) – Galloping – Stall flutter – “Whirl mode” – Potentially catastrophic 17
  • 18. Dynamic aeroelasticity: buffeting • Airfoil and non-airfoil structures • Random vibration • Usually just inconvenient 18 Laminar flow Turbulent flow (vortex shedding) Flow separation (transition region) Surface subject to turbulent flow
  • 19. Dynamic aeroelasticity: “galloping” flutter • Large amplitude, low frequency oscillation • Bluff bodies (usually non-airfoil) – Transmission lines (mostly with ice accretion) – Cable affected by vortex shedding of another cable 19
  • 20. Dynamic aeroelasticity: stall flutter • Airfoil and non-airfoil structures • Periodic (partial or complete) flow separation from the airfoil during the oscillation • Nonlinear aerodynamic reaction to the motion of the structure – Suspension bridges – Helicopter rotors (rotorcraft blades) – Turbomachinery blades • Free vortices are generated in the vicinity of the separation points • The periodic vortex shedding creates regions of reduced and even reversed velocity in the vicinity of the airfoil 20
  • 21. Dynamic aeroelasticity: “whirl mode” flutter • Two Lockheed L-188 “Electra”, – Braniff Flight 542 • September 29, 1959 • near Buffalo, TX • 34 fatalities – NW Orient Airlines Flight 710 • March 17, 1960 • near Cannelton, IN • 63 fatalities • disintegrated during flight – wing brake-up 21 Actual aircraft before crash (stinsonflyer.com) • In both cases, – No survivors – Inconclusive investigations
  • 22. “Whirl mode” flutter (a new investigation at NASA Langley) • Wind tunnel tests of an Electra 1/8- scale model showed: – Overly stiff wing – Outboard nacelles responding differently than intended – Flutter “passes on” from nacelle to (even a “flutter-free”) wing • Growing flutter magnitude decreased the oscillation frequency from 5 to 3 Hz • Wing frequency was also 3 Hz – Harmonic coupling 22 YouTube channel: NASA Langley CRGIS Flutter Tests of the Full Span Lockheed Electra
  • 23. Dynamic aeroelasticity: “whirl mode” flutter (a new investigation) 23 • According to the crash report,
  • 24. Dynamic aeroelasticity: (aeroelastic) flutter • Bending/torsion coupled motion • Self-sustained unstable motion • Antonov An-148 – March 5, 2011 (test flight) – near Garbuzovo (350 mi south of Moscow), Russia • Airspeed indicator failed (showing lower airspeed) • Pilots accelerated 70 mi/h above the design limit speed • Low-frequency vibrations created • In-flight wing break-up 24
  • 25. Dynamic aeroelasticity: non-airfoil flutter • Bending/torsion coupled motion • Self-sustained unstable motion • Tacoma Narrows Bridge – Opened to traffic on July 1, 1940 – Collapsed on November 7, 1940 – Stationary wind design limit: 160 km/h – Wind speed before failure: 60 km/h 25
  • 26. Aeroelastic flutter • Under airflow excitation, structures may exhibit aeroelastic oscillations – due to interactions of aerodynamic, elastic and inertial forces • At a critical airflow speed, lifting surfaces undergo self-sustained oscillations (linear flutter speed) – Flutter: bending/torsion coupled motion with growing amplitudes • Potentially catastrophic 26
  • 27. Aeroelastic and vibration control • Allows flight vehicles to operate beyond the traditional flutter boundaries • Improves ride qualities • Minimizes vibration fatigue damage 27 (Giurgiutiu 2000, JIMSS v. 11; Nitzsche et al 2015, JIMSS) Controlled Uncontrolled Grows until the structure fails
  • 28. Conventional passive aeroelastic control / flutter prevention • There is no universal solution • Frequent strategies – add mass or redistribute mass (‘mass balance’) – increase torsional stiffness, i.e., increase ωα – increase (or decrease) ωh/ωα if it is near one (for fixed ωα) – add damping to the structure (hydraulic dampers) – require the aircraft to be flown below its critical Mach number • Penalties – Extra weight – Non-optimized operation 28 (Dowell et al. 2015, A Modern Course in Aeroelasticity, p. 118)
  • 29. Conventional active aeroelastic control • Aerodynamic control surfaces operated by servo-hydraulic actuators • Penalties/limitations – Multiple energy conversions (mechanical, hydraulic, electrical) – Large number of parts • Potential failure sites • Extra weight – High vulnerability of the hydraulic pipes network – Limited frequency bandwidth 29 (Giurgiutiu 2000, JIMSS v. 11)
  • 30. Smart materials as an alternative (e.g., piezo actuators) • Direct conversion of electrical energy to high-frequency linear motion (mechanical energy) • Electrical energy is easier to transmit throughout the aircraft (electric lines are much less vulnerable than hydraulic pipes) 30 (Giurgiutiu 2000, JIMSS v. 11) (reverse piezoelectric effect)
  • 31. An example 31 • Active control flap for noise and vibration reduction • Piezo-stack actuators (Straub and King 1996)
  • 32. Smart materials (piezos) • Advantages – Can be embedded in the structure (e.g. on-blade actuation) – High energy/mass ratio – Direct piezoelectric effect can also be exploited • Passive and active strategies • Sensing and actuation • Energy harvesting • Disadvantages – Piezos (reverse effect) • Very small strokes (e.g. 0.1%) • Requires displacement amplification mechanisms 32
  • 33. Fixed wing aircraft studies • Heeg 1993 (NASA Langley) – Piezoelectric actuators – Flutter suppression of a rigid wing supported by springs – +20% flutter speed • McGowan et al. 1998 – 12% decrease flutter dynamic pressure – 75% decrease gust bending moment 33
  • 34. A rotating-wing application of smart materials • Feszty and Nitzsche 2011 – Carleton University, Canada • Stiffness modulation using piezoelectric actuators for vibration control in helicopters 34 (flight tested) Nitzsche et al 2015, JIMSS
  • 35. Flutter can be exploited for wind energy harvesting • Vibrations in a general sense can be exploited for energy harvesting – Direct piezoelectric effect • Flutter oscillations can provide a useful additional source of small amounts of electrical power – e.g., for embedded Structural Health Monitoring systems – Airfoil-based generators 35
  • 36. An example • The RC glider was modified to include: – two piezoelectric patches placed at the roots of the wings • to harvest energy from wing vibrations – a cantilevered piezoelectric beam installed in the fuselage • to harvest energy from rigid body motions of the aircraft 36 (SR Anton and DJ Inman, 2008)
  • 37. An airfoil model for flutter investigations 37 (Mozaffari-Jovin et al 2015, JVC) 2D problem
  • 38. How we investigate flutter in our lab 38 • 2-DOF (or 3-DOF) – Plunge (h) – Pitch (α) – (Control surface position, β) • U∞ is the airflow speed
  • 39. Experimental 2-DOF airfoil model 39 Pitch DOF wire springPlunge DOF springs (2/4)
  • 40. Numerical results and experimental tests • Linear case, U = 12 m/s • Nonlinear case (freeplay in the pitch DOF), U = 10 m/s 40 Continuous lines: experimental, dashed lines: simulation Linear: Erturk et al. (2010), Appl. Phys. Lett. 96(18) Nonlinear: Sousa et al. (2011), Smart Mater. Struct. 20(9)
  • 41. Possibilities of study for an smart airfoil/flutter model • Aeroelastic control – Classical aeroelasticity • Structural reinforcement • Mass tuning – “Smart” materials • Sensing and actuation – Piezoelectric materials – Shape memory materials • Energy Harvesting • Aeroelastic control + Energy Harvesting • Smart materials • Piezoceramics (electromechanical coupling) – Active control (actuation) – Passive (shunt damping) – Hybrid – Energy Harvesting • SMAs – Passive control (high loss factor, hysteretic damping) – Active control (stiffness and frequency variation) 41
  • 42. SMA elements can be included in the airfoil model (my current work) 42 k • Motivation: – Modify the aeroelastic behavior of the airfoil by exploiting the pseudoelastic hysteresis of SMAs SMA behavior
  • 43. Preliminary results: aeroelastic behavior with SMA springs 43
  • 44. An intermediate case is presented, 44  1 0 3 N e 11.6 m·sf U   
  • 45. Thank you! 45 Special thanks to: The University of Toledo and MIME Department, Toledo – OH/USA Dynamic and Smart Systems Lab (smartsys.eng.utoledo.edu)

Hinweis der Redaktion

  1. Boa tarde, meu nome é Vagner C..., sou aluno de mestrado no Dep. Eng. Aero, meu orientador é o Prof. Dr. Carlos...; Hoje vou apresentar uma “Análise do comportamento...”; Eu gostaria de agradecer aos membros da banca examinadora, Prof. Dr. (do ITA), Prof. Dr. Flávio Marques e Prof. Dr. Carlos De Marqui (EESC) e a todos os presentes;
  2. no sistema experimental, o acoplamento piezelétrico é introduzido no GDL de deslocamento linear; as piezocerâmicas são coladas na região do engaste das vigas de aço-mola que atribuem rigidez ao GDL de deslocamento linear; um fio-mola também atribui rigidez ao GDL de rotação;
  3. Como o modelo é desenvolvido em sua forma mais geral, todas as não linearidades possíveis neste trabalho são introduzidas nas equações de movimento; no GDL de rotação do aerofólio (pitch), a não linearidade freeplay (modelada como uma mola bilinear) pode ocorrer de maneira isolada ou combinada com uma mola cúbica do tipo hardening; no GDL de posição da superfície de controle, somente a não linearidade freeplay é considerada; no entanto, é possível combinar freeplay na superfície de controle com mola cúbica em pitch; nenhuma não linearidade é considerada no GDL de deslocamento linear (plunge) ou no domínio elétrico do problema;