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Transition to turbulence and flow control Jerome Hoepffner Fukagata lab 1

Jerome Hoepffner Fukagata lab - Redirection

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Page 1: Jerome Hoepffner Fukagata lab - Redirection

Transition to turbulence and flow control

Jerome HoepffnerFukagata lab

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Page 2: Jerome Hoepffner Fukagata lab - Redirection

Instability mechanisms

Kelvin-Helmholtz instability(inviscid)

Tollmien-Schlichting instability(viscous)

Couette and pipe are stable for all Reynolds.+

For boundary layers, transition to turbulenceis observed before critical Reynolds number

... what is the mechanism?

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Page 3: Jerome Hoepffner Fukagata lab - Redirection

Transient growth in the boundary layer

Some special disturbance can have very large effect, even if

the flow is stable

A pair of small streamwise vortices

move the flow particles in the wall normal direction:

deform the lines of streamwise velocity

➜generates streaks of high and low

streamwise velocity

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Page 4: Jerome Hoepffner Fukagata lab - Redirection

Boundary layer with incomming free-stream turbulence(LES: Philipp Schlatter, KTH)

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Page 5: Jerome Hoepffner Fukagata lab - Redirection

Energy evolution

Transition to turbulence can be caused by transient growth

It is not allways enough to compute the unstable eigenmodes... also compute the “optimal disturbances”

➡Stability analysis using optimization5

Page 6: Jerome Hoepffner Fukagata lab - Redirection

Sensor: measure skin friction/pressureActuator: blowing and suctionController: computes the feedback

How to compute the best controller K?

Flow control

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Page 7: Jerome Hoepffner Fukagata lab - Redirection

3D Swept-wing Boundary layer

No control

With control

2D Separated boundary layer

Examples:

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Page 8: Jerome Hoepffner Fukagata lab - Redirection

Swept-wing boundary layer with pointwise forcing

Real flow Flow field reconstructed using sensors

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