A. Bottaro (DICCA, Universit de Gnes) Petit djeuner du RTRA, - - PowerPoint PPT Presentation

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A. Bottaro (DICCA, Universit de Gnes) Petit djeuner du RTRA, - - PowerPoint PPT Presentation

A. Bottaro (DICCA, Universit de Gnes) Petit djeuner du RTRA, Toulouse, 6 june 2012 Georges de Mestral, 1941 Petit djeuner du RTRA, Toulouse, 6 june 2012 Petit djeuner du RTRA, Toulouse, 6 june 2012 Focus: passive/active flow control


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  • A. Bottaro (DICCA, Université de Gênes)

Petit déjeuner du RTRA, Toulouse, 6 june 2012

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Petit déjeuner du RTRA, Toulouse, 6 june 2012

Georges de Mestral, 1941

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Petit déjeuner du RTRA, Toulouse, 6 june 2012

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Penguins Sharks Seals

Focus: passive/active flow control

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Penguins Sharks Seals

Known techniques of passive/active flow control:

  • Injection of micro-bubbles and/or polymers
  • Riblets
  • Compliant walls
  • Viscosity modifier
  • Vortex generators
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Penguins Sharks Seals

Less known techniques of passive/active flow control:

  • Butterfly and moth wings microstructure

Left: electron microscope image of butterfly scales. Right: perspective view (with dimensions) with details of a scale. UL: upper lamina; LL: lower lamina; T: trabecula.

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Penguins Sharks Seals

Less known techniques of passive/active flow control:

  • Shark skin paint!

The coating that reduces drag (Fraunhofer, Bremen)

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How can we increase lift over a streamlined body at incidence by a passive technique?

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How can we reduce pressure drag behind a solid bluff body by a passive technique?

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Penguins Sharks Seals

Less known techniques of passive/active flow control: Passive, compliant hairy coating sea otter

(loutre de mer)

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How can we increase lift over a streamlined body at incidence by a passive technique?

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How can we increase lift over a streamlined body at incidence by a passive technique?

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How can we increase lift over a streamlined body at incidence by a passive technique?

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How can we increase lift over a streamlined body at incidence by a passive technique?

  • Prof. Ingo Rechenberg, TU Berlin

http://www.bionik.tu-berlin.de/institut/xs2vogel.html

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How can we increase lift over a streamlined body at incidence by a passive technique?

  • Prof. Ingo Rechenberg, TU Berlin

http://www.bionik.tu-berlin.de/institut/xs2vogel.html

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Wind tunnel tests in Genova

  • F. Negrello, Engineering Diploma work, 2010
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Wind tunnel tests in Genova

  • F. Negrello, Engineering Diploma work, 2010
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How can we increase lift over a streamlined body at incidence by a passive technique?

  • Prof. Ingo Rechenberg, TU Berlin

http://www.bionik.tu-berlin.de/institut/xs2vogel.html

Flexible, porous flaps delay stall …

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GOAL: instead of a single flexible flap, let’s model a continuous hairy/feathery coating to affect lift and drag

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  • Model mechanical properties of biological surfaces
  • Structures with large displacements and large rotations
  • Interaction between multiple structures

Coupling between a layer of oscillating

densely packed structures and a unsteady separated boundary layer Numerical challenges

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The initial configuration

fluid fluid + solid solid Circular cylinder, Re=200 Model of the layer?

Porous, anisotropic and compliant

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Case 1: bare cylinder

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Case 2: rigid wall-normal hair

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Case 3: rigid longitudinal hair

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Case 4: moving hair

Tfluid ≈ 4 Tstructure

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A projected frontal area V fluid velocity  density C = F 1/2 V A

2 d d

Drag

C drag Time (s)

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Drag (ctd.)

C drag Time (s)

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C = F 1/2 V A

2 L L

Lift

C lift Time (s)

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Lift (ctd.)

C lift Time (s)

C = F 1/2 V A

2 L L

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Aerodynamic performances

Cd Cd' Cl' St Case 1 1.3689 (1.39;1.356) 0.0274 0.4381 0.199 (0.199;0.198) Case 2 3.1464 0.1943 1.1376 0.1946 Case 3 1.3035 0.0207 0.3839 0.1916 Case 4 1.2109 0.012 0.3008 0.1661 (Bergmann et al. Phys. Fluids 2005 ; He et al J. Fluid Mech. 2000)

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Aerodynamic perf.(ctd.)

Cd Cd' Cl' St Case 1 ref ref ref ref Case 2 +130% +608% +160%

  • 2.21%

Case 3

  • 4.78%
  • 24.54%
  • 12.37%
  • 3.71%

Case 4

  • 11.54%
  • 56.09%
  • 31.34%
  • 16.53%
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Physical mechanism

Difference of time-averaged pressure field <P with hair>-<P ref>

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Physical mechanism

The hairy layer counteracts flow separation Contours of vertical velocity Movements of reference cilia Contours of vertical velocity Force field

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15% drag reduction 40% reduction in lift fluctuations

Optimal self-adaptive hairy layer

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 Simulations show a reduction of pressure drag

  • n a cylinder for a unsteady laminar flow (Re = 200).

 The motion of the hairy structures can improve aerodynamic performances  The structural parameters of the actuators have been optimised  Immediate perspectives concern flexible filaments and turbulent configurations; possible applications to small underwater vehicles and to UAV/MAV (in the aeronautical field) Favier et al., JFM 2009

Reducing pressure drag:

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In fact, a single flexible filament can do much already!!

Bagheri et al., PRL, 2012 (submitted)

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In fact, a single flexible filament can do much already!!

Bagheri et al., PRL, 2012 (submitted)

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A symmetry-breaking bifurcation occurs when vortices and structures resonate …

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increasing R2  increased rigidity of the structure

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Consider a hairfoil: the control elements (the “feathers”) must be placed in the position of largest sensitivity to achieve an effect

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NACA0012 a = 18° a = 15° Re = 104

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a = 18° a = 18°  feathers = 890 Kg/m3 (keratin)

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Summary of runs a = 15° <CD> = 0.284 <CL> = 0.579

Tfluid = 0.5 Tstructure + 1.35%

  • 13%

Tfluid = Tstructure + 2 %

  • 10%

Tfluid = 2 Tstructure + 3%

  • 9%

Tfluid= 4 Tstructure

  • 0.2 %

+ 2.5% Tfluid = 8Tstructure

  • 7 %
  • 11%

Results are similar when a = 18o, except that now <CL> increases the most when Tfluid = 2 Tstructure

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Kunze & Brücker, CRAS 2012

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Must excite

The amplitude of the oscillations decreases (the system’s stability improves) as Tstructure (i.e. m l Kr ) A parametric resonance must be triggered to optimise the response of the system

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MAV/UAV Wind turbines Hydraulic machines (cavitation?) Sound mitigation

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How can we increase lift over a streamlined body at incidence by a passive technique?

  • Prof. Ingo Rechenberg, TU Berlin

http://www.bionik.tu-berlin.de/institut/xs2vogel.html

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Biomimetic winglets

Guerrero et al., CRAS, 2012

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Biomimetic winglets

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Biomimetic winglets

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Biomimetic winglets

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Biomimetic winglets

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Advantages

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… which translate into:

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Other biomimetics secrets currently under investigation include:

  • owl silent flight

"It was just because of the surface of owl’s body have a lot of coupling interaction such as special surface morphology, unique wing configuration, special internal structure and highly flexible

  • material. They can delay the separation of turbulent boundary

layer around the airfoil profile, reduce pulsating pressure of the surface of wings, and reduce the production of sound energy. Above all the feature make the surface have function of noise elimination." (Liang et al., Adv. Natur. Sciences, 2010)

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Other biomimetics secrets currently under investigation include:

  • owl silent flight
  • tubercles on whale flipper, effect on stall, lift and drag …

Tubercle technology! Whalepower Corp., Canada

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Other biomimetics secrets currently under investigation include:

  • owl silent flight
  • tubercles on whale flipper, effect on stall
  • skin friction drag reduction with superhydrophobic surfaces

Leaves retain a air film underwater, using hydrophobic hairs with hydrophilic tips: 10% drag reduction in a large-scale ship model (Nees Institute, University of Bonn)

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… and many others …