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Entrainment and topology of accelerating shear layers

Published online by Cambridge University Press:  06 December 2016

Giuseppe A. Rosi*
Affiliation:
Department of Mechanical and Materials Engineering, Queen’s University, Kingston, ON K7L 3N6, Canada
David E. Rival
Affiliation:
Department of Mechanical and Materials Engineering, Queen’s University, Kingston, ON K7L 3N6, Canada
*
Email address for correspondence: g.rosi@queensu.ca

Abstract

A constantly accelerating circular plate was investigated towards understanding the effect of non-stationarity on shear-layer entrainment and topology. Dye visualizations and time-resolved particle image velocimetry measurements were collected for normalized accelerations spanning three orders of magnitude. Increasing acceleration acts to organize shear-layer topology. Specifically, the Kelvin–Helmholtz instabilities within the shear layer better adhered to a circular path and exhibited consistent and repeatable spacing. Normalized starting-vortex circulation was observed to collapse with increasing acceleration, which one might not expect due to increased levels of mixing at higher instantaneous Reynolds numbers. The entrainment rate was shown to increase nonlinearly with increasing acceleration. This was attributed to closer spacing between instabilities, which better facilitates the roll-up of fluid between the shear layer and vortex core. The shear-layer organization observed at higher accelerations was associated with smaller spacings between instabilities. Specifically, analogous point-vortex simulations demonstrated that decreasing the spacing between instabilities acts to localize and dampen perturbations within an accelerating shear layer.

Type
Papers
Copyright
© 2016 Cambridge University Press 

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References

Ashbee, T. L., Esler, J. G. & McDonald, N. R. 2013 Generalized hamiltonian point vortex dynamics on arbitrary domains using the method of fundamental solutions. J. Comput. Phys. 246, 289303.Google Scholar
Brown, G. L. & Roshko, A. 1974 On density effects and large structure in turbulent mixing layers. J. Fluid Mech. 64 (4), 775816.CrossRefGoogle Scholar
Cantwell, B. & Coles, D. 1983 An experimental study of entrainment and transport in the turbulent near-wake of a circular cylinder. J. Fluid Mech. 136, 321374.Google Scholar
Caulfield, C. P., Yoshida, S. & Peltier, W. R. 1996 Secondary instability and three-dimensionalization in a laboratory accelerating shear layer with varying density differences. Dyn. Atmos. Oceans 23 (1), 125138.CrossRefGoogle Scholar
Chauhan, K., Philip, J., de Silva, C. M., Hutchins, N. & Marusic, I. 2014 The turbulent/non-turbulent interface and entrainment in a boundary layer. J. Fluid Mech. 742, 119151.Google Scholar
Corrsin, S. & Kistler, A. L.1955 Free-stream boundaries of turbulent flows. NACA Tech. Rep.Google Scholar
Dabiri, J. O. & Gharib, M. 2004 Fluid entrainment in isolated vortex rings. J. Fluid Mech. 511, 311331.Google Scholar
Didden, N.1977 Untersuchung laminarer, instabiler Ringwirbel mittels Laser Doppler Anemometrie. Mitteilungen aus dem Max-Planck-Institut für Strömungsforschung. Dt. Forschungs- u. Versuchsanst. für Luft- u. Raumfahrt e.V., Forschungszentrum Aerodynam. Versuchsanst. Göttingen.Google Scholar
Dimotakis, P. E. & Brown, G. L. 1976 The mixing layer at high Reynolds number: large-structure dynamics and entrainment. J. Fluid Mech. 78, 535560.CrossRefGoogle Scholar
Gharib, M., Rambod, E. & Shariff, K. 1998 A universal time scale for vortex ring formation. J. Fluid Mech. 360, 121140.Google Scholar
Glezer, A. 1988 The formation of vortex rings. Phys. Fluids 31 (12), 35323542.Google Scholar
Hain, R. & Kaehler, C. J. 2007 Fundamentals of multiframe particle image velocimetry (PIV). Exp. Fluids 42 (4), 575587.Google Scholar
Ho, C. M. & Huerre, P. 1984 Perturbed free shear layers. Annu. Rev. Fluid Mech. 16 (1), 365422.CrossRefGoogle Scholar
Krug, D., Holzner, M., Lüthi, B., Wolf, M., Kinzelbach, W. & Tsinober, A. 2013 Experimental study of entrainment and interface dynamics in a gravity current. Exp. Fluids 54 (1530), 113.Google Scholar
Liess, C. & Didden, N. 1976 Experimente zum einflu und der anfangsbedin-gungen auf die instabilitat von ringwirbeln. Z. Angew. Math. Mech. 56, 625639.Google Scholar
Mistry, D., Philip, J., Dawson, J. R. & Marusic, I. 2016 Entrainment at multi-scales across the turbulent/non-turbulent interface in an axisymmetric jet. J. Fluid Mech. 802, 690725.Google Scholar
Olcay, A. B. & Krueger, P. S. 2008 Measurement of ambient fluid entrainment during laminar vortex ring formation. Exp. Fluids 44 (2), 235247.Google Scholar
Olcay, A. B. & Krueger, P. S. 2010 Momentum evolution of ejected and entrained fluid during laminar vortex ring formation. Theor. Comput. Fluid Dyn. 24 (5), 465482.Google Scholar
Pawlak, G. & Armi, L. 1998 Vortex dynamics in a spatially accelerating shear layer. J. Fluid Mech. 376, 135.CrossRefGoogle Scholar
Pawlak, G. & Armi, L. 2000 Mixing and entrainment in developing stratified currents. J. Fluid Mech. 424, 4573.Google Scholar
Phillip, J. & Marusic, I. 2012 Large-scale eddies and their roles in entrainment in turbulent jets and wakes. Phys. Fluids 48, 055108.Google Scholar
Ricou, F. P. & Spalding, D. B. 1961 Measurements of entrainment by axisymmetrical turbulent jets. J. Fluid Mech. 11, 2132.Google Scholar
Saffman, P. G. 1978 The number of waves on unstable vortex rings. J. Fluid Mech. 84 (04), 625639.CrossRefGoogle Scholar
Schlatter, P., Li, Q., Brethouwer, G., Johansson, A. V. & Henningson, D. S. 2010 Simulations of spatially evolving turbulent boundary layers up to Re𝜃 = 4300. Intl J. Heat Fluid Flow 31 (3), 251261.CrossRefGoogle Scholar
Shadden, S. C., Dabiri, J. O. & Marsden, J. E. 2006 Lagrangian analysis of fluid transport in empirical vortex ring flows. Phys. Fluids 18, 047105.CrossRefGoogle Scholar
Shadden, S. C., Katija, K., Rosenfeld, M., Marsden, J. E. & Dabiri, J. O. 2007 Transport and stirring induced by vortex formation. J. Fluid Mech. 593, 315331.CrossRefGoogle Scholar
da Silva, C. B., Dos Reis, R. J. N. & Pereira, J. C. F. 2011 The intense vorticity structures near the turbulent/non-turbulent interface in a jet. J. Fluid Mech. 685, 165190.Google Scholar
Wolf, M., Holzner, M., Krug, D., Lüthi, B., Kinzelbach, W. & Tsinober, A. 2013 Effects of mean shear on the local turbulent entrainment process. J. Fluid Mech. 731, 95116.Google Scholar
Xu, L. & Nitsche, M. 2015 Start-up vortex flow past an accelerated flat plate. Phys. Fluids 27 (3), 033602.Google Scholar

Rosi and Rival supplementary movie

Shear-layer dye visualizations for the low- and mid-acceleration cases (top and bottom sequences, respectively) over a diameters-traveled domain of 0 ≤ s/D ≤ 4.9. Circulation-based Reynolds numbers are provided as well.

Download Rosi and Rival supplementary movie(Video)
Video 10.9 MB

Rosi and Rival supplementary movie

Enstrophy fields for low-, mid- and high-acceleration cases (first, second and third rows, respectively) over a diameters-traveled domain of 0.7 ≤ s/D ≤ 1.0. Enstrophy fields from single runs are presented in the first, second and third columns, while the fourth column presents the 30-run, phase-averaged enstrophy fields. Circulation-based Reynolds numbers are indicated as well.

Download Rosi and Rival supplementary movie(Video)
Video 11.4 MB

Rosi and Rival supplementary movie

Enstrophy-containing mass regions (red) identified using area thresholds of ΔA=2%. Regions of entrainment and detrainment are indicated by blue and green arrows, respectively.

Download Rosi and Rival supplementary movie(Video)
Video 11.3 MB