Prof. Jean-Marc Moschetta Professor of Aerodynamics

Mar 15, 2008 - for true hovering capabilities and still maintain high cruise speed for covertness. Several combinations of ... Camber changes h = 3-9% with synchronous change of reflex h i. = 1-3% ..... autonomous mode. • Tilt-body better ...
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Prof. Jean-Marc Moschetta Professor of Aerodynamics Department of Aerodynamics Energetics and Propulsion ISAE BP54032, 31055 Toulouse Cedex France [email protected]. Hovering Capabilities of Fixed-Wing Micro-Aerial Vehicles Jean-Marc Moschetta1, Institut Supérieur de l’Aéronautique et de l’Espace, Université de Toulouse, France and Sergey V. Shkarayev2, Department of Aerospace and Mechanical Engineering, University of Arizona, Tucson, Arizona

Fixed-wing micro air vehicles (MAV) are very attractive for outdoor surveillance missions since they generally offer better payload and endurance capabilities than rotorcraft or flapping-wing vehicles of equal size. They are generally less challenging to control than rotorcraft in outdoor environment and allow for a dash capability to escape enemy attention. On the other hand, they usually fail miserably to perform vertical take-off and landing (VTOL) and sustain stable hover flight which proves to be crucial for urban surveillance missions including building intrusion. The present paper investigates the possibility to improve the aerodynamic performance of fixed-wing MAV concepts so as to allow for true hovering capabilities and still maintain high cruise speed for covertness. Several combinations of rotors and fixed-lifting surfaces were tested, analyzed and compared. First, a tandem-rotor biplane MAV configuration was designed and tested as a result of different biplane powered configurations. A low-speed autonomous fixed-wing MAV was fabricated and flight tested to perform multi-tasking outdoor surveillance missions. Secondly a side-by-side comparison of a tiltwing and a tilt-body powered configuration with a pair of counter-rotating motors in tractor configuration with MAV configurations were carried out. The tilt-body configuration was shown to be more suitable for MAV applications with higher hovering performances. Second, a coaxial tilt-body concept based on coaxial motors and contra-rotating propellers inspired from the Convair XFY1 “Pogo” experimental aircraft was designed and tested. A wind tunnel test was carried out to fully characterize the aerodynamic performances of the coaxial tail-sitter configuration, named Vertigo. An autonomous version was developed in order to autonomously perform transitions between horizontal and vertical flight. A smaller 300-mm span version, called mini-Vertigo, was designed and fabricated based on a series of wind tunnel tests using miniaturized coaxial-rotor propulsion set. Autonomous altitude hold and attitude stability augmentation were then achieved using specific control laws adapted for the Paparazzi autopilot system. Thirdly, a new no-through-shaft coaxial-rotor configuration has been proposed in order to enhance the prototype ruggedness through an embedded spherical structure made of carbon rods. It is believed that such a crash-proof VTOL MAV, called Cyclope, can be very attractive for the use of MAV systems in real operations and allows for further size reduction such as for Nano Air Vehicles applications. Current prospects include both further wind tunnel tests using new high-precision micro sting-balances on coaxial-rotor tail-sitter MAVs and the development of control laws to autonomously perform transition flights. 1

Professor of Aerodynamics, Department of Aerodynamics, Energetics and Propulsion, ISAE BP54032, 31055 Toulouse Cedex, France, jean-

[email protected]. 2

Associate Professor, Department of Aerospace and Mechanical Engineering, The University of Arizona, PO Box 210119, Tucson AZ 85721-

00119,[email protected].

1st US-Asian Demonstration & Assessment of Micro-Aerial & Unmanned Ground Vehicle Technology, 10-15 March, Agra, India

Hovering Capabilities of Fixed-Wing Micro Air Vehicles Jean-Marc Moschetta Institut Supérieur de l’Aéronautique et de l’Espace, Toulouse, France Sergey Shkarayev University of Arizona, Tucson, Arizona

Motivation Typical MAV mission profile Phase 1

Phase 2 Loiter

Dash Phase 3 Hover

Launch

Building intrusion Phase 4 March 10-15, 2008

MAV’08

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MAV design challenges Rotorcraft MAVs

Fixed Wing MAVs MinusKiool (2003)

Br2C (2007)

20 cm, 60 g 36 cm, 490 g

Poor image capturing • Maneuverability in confined environment •

Challenging to control • Fast horizontal flight •

• VTOL Fixed-Wing MAV – High speed for covertness – Low speed for clear images – Limited electric consumption March 10-15, 2008

MAV’08

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A low-speed in-flight adaptive wing MAV Camber changes h = 3-9% with synchronous change of reflex hi = 1-3%

Test flights were conducted with Pitot tube sensor With camber increases from 3% to 9% minimal speed decreases by about 100% March 10-15, 2008

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A low-speed tandem wing MAV

• Tandem-wing MAV • Gimbaled 2-axis camera

TYTO Moschetta, Thipyopas, J Aircraft, vol. 44, 2007 March 10-15, 2008

250g - 40 cm MAV’08

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New MAV concepts Tilt-rotor

Tilt-body Tilt-wing March 10-15, 2008

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Experimental setup • Wind tunnel

l

– Test section 45 x 45cm – Velocity 2-20 m/s

Pivot Point

r

Aft Strut always perpendicular to the model longitudinal axis

• Measurements

Left Strut Right Strut

LC5 LC3

– Improved 5-component balance :

Adjustable plate controlled by motor to change AoA. LC6 LC2

• force 0.004 N • moment 0.002 N.cm

Free Stream Velocity

LC4 LC1

Motor

Ground LC1 – 4 are fixed onto the ground, LC5 - 6 are supported by adjustable plate and always rotate with the model

Kochersberger, AIAA paper 2005-4759 Suharyono, Aerospace Sc. & Tech., 2006 March 10-15, 2008

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Future MAV wind tunnel (2009) 6-component sting micro-balance: 8-mm diameter, 100g max load,

Variable-pitch fan

Test section 120 x 80 cm Contraction ratio 10:1 Turbulence 0.3% Speed 0 - 25 m/s Test section length 2.5 m Length 19 m Width 4.5 m Height 7 m March 10-15, 2008

MAV’08

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Tilt-wing vs. tilt-body 30°

• Speed 0-15 m/s • tilt angles 0°, 30°, 60°, 90° • PWM signal 40, 60, 80, 100% • Struts corrections (AoA, speed)

60°

Tilt-body (0°) March 10-15, 2008

MAV’08

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α TW = α TB = α Tilt-body

S Λ , 2 2

S, Λ

LTB = qS ×

(Di )TB

=

πΛ 2

(α − α 0 )

1 2 qS πΛ × (α − α 0 ) 4

March 10-15, 2008

Tilt-wing

LTW = 2 q

(Di )TW MAV’08

=

S πΛ (α − α 0 ) = 1 × LTB × 2 4 2

1 1 2 qS πΛ × (α − α 0 ) = × (Di )TB 8 2 10

LTW = LTB = W Tilt-body

S Λ , 2 2

S, Λ

LTB = qS ×

πΛ 2

Tilt-wing

(α TB − α 0 ) = W

LTW = 2 q

S πΛ (α TW − α 0 ) = W × 2 4

α TW = 2α TB − α 0

(Di )TB

=

1 2 qS πΛ × (α TB − α 0 ) 4

March 10-15, 2008

(Di )TW MAV’08

=

1 2 qS πΛ × (α TW − α 0 ) = 2 × (Di )TB 8 11

Tilt-wing vs. tilt-body Downward force

100

90

Lift = Weight Drag = Thrust

80 70 60

tilt body

80

tilt body

PWM Signal (%)

Tilt angle or angle of attack (deg)

tilt wing

tilt wing

50

40 30 20

60

40

20

10 0

0 0

5

10

15

20

0

Velocity (m/s)

10

15

20

Velocity (m/s)

Tilt-wing requires more power near hover

Tilt-wing may benefit from vortical lift effects March 10-15, 2008

5

MAV’08

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Tilt-wing vs. tilt-body 0,001 0 0

5

10

15

20

-0,001

tilt wing

dM(CG)/dAoA

-0,002

tilt body

-0,003 -0,004

• « CG » located at 10% chord ahead of the AC at 16 m/s • Each gradient calculated around equilibrium points • Longitudinal stability greatly reduced at low speeds

-0,005 -0,006 -0,007

• Tilt-wing / tilt-body MAV configurations very comparable

-0,008 -0,009

Velocity (m/s)

March 10-15, 2008

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A coaxial tail-sitter mini-UAV • Tilt-body • Coaxial rotor in tractor configuration • Autonomous transition flight • rotor 500 mm • weight 1.6 kg (incl. IMU, GPS, Modem…) Convair « Pogo » XFY-1

ISAE « Vertigo » mini-UAV

(1954)

(2006)

March 10-15, 2008

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Wind tunnel measurements 1,2 1 0,8 0,6

CL

0,4 0,2 0 -0,2

Stall angle

-0,4 -0,6 -20

• Sting-mounted model

0

20

40

60

80

AoA°

• Speed 0, 5, 10, 15, 20 m/s

• strong vortical effects on wing-alone tests

• AoA -10°to 90°, sideslip

• CD0 = 0.054, L/Dmax = 4

• flap efficiency, throttle

• CL > 0.8 at AoA 15°-55°

March 10-15, 2008

100

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Coaxial tail-sitter 0,1 0,05 0

CM@CG

-0,05 -0,1 -0,15 -0,2

stall angle

-0,25 -0,3 -20

0

20

40

60

80

100

AoA°

• Stabilizing vortical effects (low aspect-ratio) • Constant pitching moment gradient after stall (CoP) March 10-15, 2008

MAV’08

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14

• Balanced lift and drag

10

V(m/s)

Powered tests

12

(V, AoA, throttle)

8 6 4 2 0 0

20

30

40

50

60

70

80

90

100

Ao A °

1,8

0,18

1,6

0,16

1,4

• Equilibrium found throughout transition

0,14

Aircraft horizontal force Aircraft vertical force

Forces (daN)

1,2

0,12

Propeller horizontal force Propeller vertical force

1,0

0,10

Aircraft pitching moment Propeller pitching moment

0,8

0,08

0,6

0,06

• Aircraft pitching moment almost constant in transition (flap efficiency)

0,4

0,04

0,2

0,02

March 10-15, 2008

0,0 0

10

MAV’08 20 30

40

50

60

70

80

90

17 0,00 100

Pitching moment (daN.m)

• Propeller-alone tests carried out to evaluate propellers contribution during transition

• Propeller-induced noseup pitching moment (side force)

10

14

Propeller-wing interaction

12

exp.

V, m/s

10

T

+

model

8 6 4

α V

2

2w VR

αS

0 10

20

30

40

50 60 AoA, deg

70

80

90

McCormick

 w   w0

4

3

  w V  w  + 2  cos α +     w0  w0  w0  2

2

V   w0

2

  = 1 

V   w  VR w =  +2 cos α  +  2 sin α  w0 w0  w0   w0 

2



 w w0 sin α   w0 VR 

α S = sin −1  2

Acknowledgement: Boris Bataillé & Damien Poinsot, ISAE & ONERA, Toulouse March 10-15, 2008

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Simulation of transition flight 20

14

15

12

10

Delta m, deg

10 Velocity, m/s

AoAw, deg

15

8 6 4

5

20

30

40

50 60 AoA, deg

70

80

Effective wing AoA

90

0 10

5

V Vr

2 0 10

10

20

30

40

50 AoA

60

70

80

90

0 10

20

Relative wind speed

30

40

50 60 AoA, deg

70

80

Flap deflection

• Unstalled wing (stall angle 23°) • Flap efficiency throughout transition Poinsot et al., VTOL conference, RAeS 2008 March 10-15, 2008

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90

Mini Vertigo

Dual motor-propeller

50 g

3-cell Li-Poly batteries

60 g

Speed controller & receiver

16 g

Gyros & servos

22 g

Airframe 44 g ------------------------------------------------Total weight 192 g

Fiberglass, 1 ply/side

2 Bolts, D2 Plastic insert

Fiberglass 2 plies/side

Motor mount Carbon tube 6 mm 46

Battery cell RC Receiver

200

Speed controller

Carbon tube 3 mm

Servo

March 10-15, 2008

300

Elevon

Gyro-stabilized prototype (2007) MAV’08

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Scaling effects MAV

Size (cm)

Shkarayev et al., J Aircraft (submitted), 2007

Rec

Λ

S (dm²)

m (g)

m/S (g/dm²)

Vertigo

65

16 x 104

1.80

24

1600

67

Mini-Vertigo

30

4 x 104

1.91

5

160

32

• Mini-Vertigo used high-pitch counter-rotating propellers (low RPM) • Power loading (PL) includes motor efficiency MAV

Drotor (mm)

T (N)

DL (N/m2)

P (W)

PL (W/N)

Pind (W)

Vertigo

500

15.7

80

165

10.5

90

Mini-Vertigo

140

1.55

101

45

29.0

8.2

March 10-15, 2008

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Conclusions • Tilt-body MAV configurations combining

tandem/coaxial rotors and fixed wings are promising candidates for complex outdoor/indoor surveillance missions in autonomous mode • Tilt-body better than tilt-wing MAV • Coaxial tail-sitter allows for balanced transition

March 10-15, 2008

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Current prospects: nanorotors

• Weight decreases with size as

W = 17.884 d 1.535

• FoM and power loading decrease with size (XROTOR) March 10-15, 2008

MAV’08

Acknowledgements Liu Zhen, PhD candidate, ISAE, Feb. 2008 23

Current prospects: autonomy

• Step 1: altitude/attitude hold • Step 2: autonomous transition Acknowledgements Roman Krashanitsa, Univ. Arizona, 2007 March 10-15, 2008

MAV’08

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Current prospects : improved airframe Vision (35 cm, 450 g)

• Embedded coaxial fixed-wing • No through-shaft system • Roll & fly

MAV’07, Toulouse, France, sept. 2007 Acknowledgements Dominique Bernard, ISAE, 2007 March 10-15, 2008

Frankfurt, Germany, oct. 2007 MAV’08

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Thank you

Cyclope (20 cm, 100g)

March 10-15, 2008

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