time resolved, near wall piv measurements in a high ... · we report on near wall measurements of a...

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16TH EUROPEAN TURBULENCE CONFERENCE, 21-24 AUGUST, 2017, STOCKHOLM,SWEDEN TIME RESOLVED, NEAR WALL PIV MEASUREMENTS IN A HIGH REYNOLDS NUMBER TURBULENT PIPE FLOW Christian Willert 1 , Joachim Klinner 1 , Julio Soria 2 , Omid Amili 2 , Michael Eisfelder 2 , Michel Stanislas 3 , Christophe Cuvier 3 , Gabriele Bellani 4 , Tommaso Fiorini 4 & Alessandro Talamelli 4 1 DLR Institute of Propulsion Technology, 51170 Köln, Germany 2 Monash University, Australia, 3 LML, Ecole Centrale de Lille, France, 4 University of Bologna, Italy We report on near wall measurements of a turbulent pipe flow at shear Reynolds numbers up to Re τ = 40000 acquired in the CICLoPE facility near Bologna, Italy. With 900 mm diameter and 110 m length the facility offers a well-established turbulent flow with viscous length scales ranging from y + = 85 μm at Re τ = 5000 to y + = 11 μm at Re τ = 40000. These length scales can be resolved with a high-speed PIV camera at image magnification near unity. For the PIV mea- surements the light of a high-speed, double-pulse laser is focused into a 300 μm thin light sheet that is introduced radially into the pipe. The light scattered by 1 μm water-glycerol droplet seeding is observed from the side by the camera via a 1 mm thin high-aspect ratio mirror with a field of view covering 20 mm in wall-normal and 5 mm in stream-wise direction (Fig. 1, right). Facility vibrations of up to 50μm peak-to-peak could be accounted for with image processing thereby providing measurements with a spatial resolution at the wall unit level (Fig. 2, left). Statistically converged ve- locity profiles could be achieved using up to 70000 samples per sequence acquired at low laser repetition rates (100 Hz). Higher sampling rates of 10 kHz provide temporally coherent data from which frequency spectra can be derived. Prelim- inary analysis of the data shows a well resolved inner peak that grows with increasing Reynolds number (Fig. 2, right). Figure 1. PIV-setup on the CICLoPE facility (left), insert for near-wall PIV measurements (right) Figure 2. Left: mean streamwise velocity scaled with inner coordinates. Right: variances and co-variances of the streamwise and wall-normal velocity components. DNS turbulent channel flow data from Lee & Moser, JFM 774 (2015) Acknowledgment: This EuHIT Project was funded by the European Community Framework Programme 7, Grant Agree- ment no. 312778, https://www.euhit.org/projects/HoloPipe

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Page 1: TIME RESOLVED, NEAR WALL PIV MEASUREMENTS IN A HIGH ... · We report on near wall measurements of a turbulent pipe flow at shear Reynolds numbers up to Re ... These length scales

16TH EUROPEAN TURBULENCE CONFERENCE, 21-24 AUGUST, 2017, STOCKHOLM, SWEDEN

TIME RESOLVED, NEAR WALL PIV MEASUREMENTS IN A HIGH REYNOLDS NUMBERTURBULENT PIPE FLOW

Christian Willert1, Joachim Klinner1, Julio Soria2, Omid Amili2, Michael Eisfelder2, Michel Stanislas3,Christophe Cuvier3, Gabriele Bellani4, Tommaso Fiorini4 & Alessandro Talamelli4

1DLR Institute of Propulsion Technology, 51170 Köln, Germany2Monash University, Australia, 3LML, Ecole Centrale de Lille, France, 4University of Bologna, Italy

We report on near wall measurements of a turbulent pipe flow at shear Reynolds numbers up to Reτ = 40000 acquired inthe CICLoPE facility near Bologna, Italy. With 900 mm diameter and 110 m length the facility offers a well-establishedturbulent flow with viscous length scales ranging from y+ = 85µm at Reτ = 5000 to y+ = 11µm at Reτ = 40000.These length scales can be resolved with a high-speed PIV camera at image magnification near unity. For the PIV mea-surements the light of a high-speed, double-pulse laser is focused into a ≈ 300µm thin light sheet that is introducedradially into the pipe. The light scattered by 1µm water-glycerol droplet seeding is observed from the side by the cameravia a 1 mm thin high-aspect ratio mirror with a field of view covering 20 mm in wall-normal and 5 mm in stream-wisedirection (Fig. 1, right). Facility vibrations of up to 50µm peak-to-peak could be accounted for with image processingthereby providing measurements with a spatial resolution at the wall unit level (Fig. 2, left). Statistically converged ve-locity profiles could be achieved using up to 70000 samples per sequence acquired at low laser repetition rates (100 Hz).Higher sampling rates of 10 kHz provide temporally coherent data from which frequency spectra can be derived. Prelim-inary analysis of the data shows a well resolved inner peak that grows with increasing Reynolds number (Fig. 2, right).

Figure 1. PIV-setup on the CICLoPE facility (left), insert for near-wall PIV measurements (right)

100 101 102 103 104

y +

0

5

10

15

20

25

30

U+

= 0.41B= 5.1

u + = 1/ log(y + ) +B

DNS Reτ = 5200

Reτ = 5386

Reτ = 11729

Reτ = 19918

Reτ = 27997

Reτ = 39985

100 101 102 103 104

y +

2

0

2

4

6

8

10

12

<u′ iu′ j> < u ′u ′ >

<v ′v ′ >

<u ′v ′ >

DNS Reτ = 5200

Reτ = 5386

Reτ = 11729

Reτ = 19918

Reτ = 27997

Reτ = 39985

Figure 2. Left: mean streamwise velocity scaled with inner coordinates. Right: variances and co-variances of the streamwise andwall-normal velocity components. DNS turbulent channel flow data from Lee & Moser, JFM 774 (2015)

Acknowledgment: This EuHIT Project was funded by the European Community Framework Programme 7, Grant Agree-ment no. 312778, https://www.euhit.org/projects/HoloPipe