03.06.2013 Views

Abstracts - KTH Mechanics

Abstracts - KTH Mechanics

Abstracts - KTH Mechanics

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

Assessment of a wavelet based coherent structure eduction<br />

technique in turbulent wall flows.<br />

R. Camussi a, W. Da Riz a<br />

The aim of the work is to present an assessment of a wavelet based method for<br />

identifying coherent structures (CS) from 2D PIV data in turbulent wall flows.<br />

The database used is provided by Adrian and co-workers<br />

(http://ltcf.tam.uiuc.edu/) and previously used in Adrian et al. 1 for high and low<br />

Reynolds number flows (Re = 1015/7705, = 8.84/10.35 mm).<br />

The algorithm is based on wavelet analysis of 2D PIV velocity field (Camussi 2) and<br />

validated against a method based on the swirling strength (Zhou et al. 3). An algorithm<br />

for the computation of the velocity gradient tensor at each point of the 2D PIV<br />

velocity field has been implemented: the CS has been identified as to be the area<br />

where the velocity gradient tensor has a pair of conjugate complex eigenvalues with<br />

squared imaginary part ci 2 overcoming a fixed threshold equals to std(ci 2). The<br />

algorithm for CS identification via wavelet analysis is based on the LIM indicator<br />

(Farge 4, Camussi and Guj 5); here only the velocity component normal to the wall has<br />

been used. The CS has been identified as the point where the maximum value of LIM<br />

over all wavelet scales shows a relative peak. Statistics of CS identified by means of the<br />

two methods revealed no substantial differences for negative-vorticity structure, and a<br />

relationship between wavelet wavelength and vortex size has been carried out (Fig. 1a).<br />

For positive-vorticity structures the analysis of results shown striking differences<br />

arising from the fact that the LIM based algorithm tends to identify negative-vorticity<br />

vortex packets (Fig. 1-b circled), which form a zone of local positive vorticity (Fig. 1-b<br />

red) along with positive-vorticity structures. Similarities and differences between high<br />

and low Re flows are also shown.<br />

a Mechanical and Industrial Engineering Department, University “ROMA TRE”, Rome, Italy.<br />

1 Adrian, R. J.,Meinhart C. D., Tomkins C., J. Fluid Mech. 422, 1–53 (2000).<br />

2 Camussi R., Exps. Fluids, 32, 76-86 (2002).<br />

3 Zhou, J., Adrian, R.J., Balachandar S., Kendall T.M., J. Fluid Mech. 387, 353-396 (1999).<br />

4 Farge M., Annual Review of Fluid <strong>Mechanics</strong>, 24, 395-457 (1992).<br />

5 Camussi R., Guj G., J. Fluid Mech. 348, 177-199 (1997).<br />

(a)<br />

y (mm)<br />

45<br />

40<br />

35<br />

30<br />

25<br />

20<br />

15<br />

10<br />

5<br />

10 20 30 40<br />

x(mm)<br />

Fig. 1: (a) r0 vs. wavelength. (b) Mean velocity field vorticity (wavelength = 26.6 mm)<br />

(b)<br />

159

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!