Transcript
Page 1: Milan Milovanovic, Marek Gayer, Joris Michielsen and Ole Morten Aamo

1

Milan Milovanovic, Marek Gayer, Joris Michielsen and Ole Morten Aamo

48th IEEE Conference on Decision and Control, CDC 2009, Shanghai, China

Model-based Stabilization of Vortex Shedding with CFD Verification

Page 2: Milan Milovanovic, Marek Gayer, Joris Michielsen and Ole Morten Aamo

2

Von Kármán vortex street:

Page 3: Milan Milovanovic, Marek Gayer, Joris Michielsen and Ole Morten Aamo

3

for , with boundary conditions

and

A complex Ginzburg-Landau equation:

),0( dxx

)(),0( tutA 0),( txA d

2

1 2 32( ) ( )

A A Aa a x a x A

t x x

Page 4: Milan Milovanovic, Marek Gayer, Joris Michielsen and Ole Morten Aamo

4

With the control input:

A complex Ginzburg-Landau equation becomes:

for with boundary conditions:

( ) ( )

( ) ( )t R xx R I xx I

t I xx I R xx R

a b x a b x

a b x a b x

0,1x

(0, ) 0, (0, ) 0

(1, ) , (1, ) ( )R I

t t

t u t u t

1

1 ,10

1

,1 10

[ ( ) ( , ) ( ) ( , )] ,

[ ( ) ( , ) ( ) ( , )]

R c

I c

u k y y t k y y t dy

u k y y t k y y t dy

Page 5: Milan Milovanovic, Marek Gayer, Joris Michielsen and Ole Morten Aamo

5

Looking for:

to transform sistem into:

for with boundary conditions:

0

0

( , ) ( , ) [ ( , ) ( , ) ( , ) ( , )]

( , ) ( , ) [ ( , ) ( , ) ( , ) ( , )]

x

c

x

c

x t x t k x y x t k x y y t dy

x t x t k x y x t k x y y t dy

( ) ( )

( ) ( )t R xx R I xx I

t I xx I R xx R

a f x a f x

a f x a f x

0,1x

(0, ) (0, ) (1, ) (1, ) 0.t t t t

Page 6: Milan Milovanovic, Marek Gayer, Joris Michielsen and Ole Morten Aamo

6

The pair of kernels and satisfy the PDEs:

( , )k x y ( , )ck x y

, ,

( , ) ( , ) ,

( , ) ( , )

xx yy c c

c xx c yy c c

k k x y k x y k

k k x y k x y k

for with boundary conditions:

( , ) , : 0 1 ,x y x y y x

0

0

1( , ) ( , ) , ( ,0) 0,

21

( , ) ( , ) , ( ,0) 0,2

x

x

c c c

k x x d k x

k x x d k x

where

2 2

2 2

( ) ( ) ( ) ( )( , ) ,

( ) ( ) ( ) ( )( , ) .

R R R I I I

R I

R I I I R R

R I

a b y f x a b y f xx y

a a

a b y f x a b y f xx y

a a

Page 7: Milan Milovanovic, Marek Gayer, Joris Michielsen and Ole Morten Aamo

7

Simulation setup

Page 8: Milan Milovanovic, Marek Gayer, Joris Michielsen and Ole Morten Aamo

8

Measurement curves:

Suction/blowing actuation slots:

Page 9: Milan Milovanovic, Marek Gayer, Joris Michielsen and Ole Morten Aamo

9

GL parameters:

Page 10: Milan Milovanovic, Marek Gayer, Joris Michielsen and Ole Morten Aamo

10

The residue between real CFD data and GL simulations:

Page 11: Milan Milovanovic, Marek Gayer, Joris Michielsen and Ole Morten Aamo

11

Controller kernels:

Page 12: Milan Milovanovic, Marek Gayer, Joris Michielsen and Ole Morten Aamo

12

The state feedback controller:

1 ,10

201

1( ) ( , )

1exp ( )

2

dx d dc

d d d

x

x x x xu t k ik A x t

x x x

a d dxa

Page 13: Milan Milovanovic, Marek Gayer, Joris Michielsen and Ole Morten Aamo

13

Transverse velocity:

Page 14: Milan Milovanovic, Marek Gayer, Joris Michielsen and Ole Morten Aamo

14

The control input:

Page 15: Milan Milovanovic, Marek Gayer, Joris Michielsen and Ole Morten Aamo

15

Stabilization of fully developed vortex shedding at Re=60:

Page 16: Milan Milovanovic, Marek Gayer, Joris Michielsen and Ole Morten Aamo

16

Conclusion:• Vortex shedding is successfully removed by the

control at Reynolds number Re=60.• The link is established between controllers previously

designed for the Ginzburg-Landau model of vortex shedding and the actual flow dynamics.

Additional effort:• Ongoing work: trying for Re>60• Future work: involve CFD verification of the output

feedback problem, which was solved for the GL equation in [Aamo2007]


Top Related