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Turbulent flow over a backward-facing step. Part 1. Effects of anti-cyclonic system rotation

Published online by Cambridge University Press:  06 December 2010

MUSTAFA BARRI*
Affiliation:
Fluids Engineering Division, Department of Energy and Process Engineering, Norwegian University of Science and Technology (NTNU), 7491 Trondheim, Norway
HELGE I. ANDERSSON
Affiliation:
Fluids Engineering Division, Department of Energy and Process Engineering, Norwegian University of Science and Technology (NTNU), 7491 Trondheim, Norway
*
Email address for correspondence: barri@ntnu.no

Abstract

The effects of rotation on turbulent flow with separation and reattachment are investigated by means of direct numerical simulations. The backward-facing step configuration is rotated about a spanwise axis such that the sudden expansion of the channel is on the pressure side. The upstream flow is a fully developed plane Poiseuille flow subjected to orthogonal-mode rotation, which subsequently detaches from the step corner and eventually reattaches further downstream. The size of the resulting separation bubble with recirculating flow diminishes monotonically with increasing rotation rates and the reattachment distance is reduced from about 7 to 3 step heights. This is ascribed to the augmentation of the cross-stream turbulence intensity in the anti-cyclonic shear layer formed between the bulk flow and the recirculating eddy due to the destabilizing influence of the Coriolis force. The spanwise-oriented vortex cells or roller eddies found in non-rotating shear layers were disrupted by the enhanced turbulence. The flow along the planar wall is subjected to an adverse pressure gradient induced by the sudden expansion. The stabilizing influence of the system rotation in this cyclonic shear layer tends to damp the turbulence, the flow becomes susceptible to flow separation, and a substantial cyclonic recirculation bubble is observed at the highest rotation rates. The resulting meandering of the bulk flow is associated with interactions between the anti-cyclonic shear layer at the stepped side and the cyclonic shear flow along the planar surface. These give rise to enhanced turbulence levels at the cyclonic side in spite of the otherwise stabilizing influence of the Coriolis force. Exceptionally high velocity fluctuations in the spanwise direction are observed in the vicinity of flow reattachment behind the step and ascribed to longitudinal Taylor–Görtler-like roll cells which extend into the backflow region. These roll cells arise from a centrifugal instability mechanism associated with the convex streamline curvature in the reattachment zone.

Type
Papers
Copyright
Copyright © Cambridge University Press 2010

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References

REFERENCES

Andersson, H. I. & Kristoffersen, R. 1995 Turbulence statistics of rotating channel flow. In Turbulent Shear Flows 9 (ed. Durst, F., Kasagi, N., Launder, B. E., Schmidt, F. W., Suzuki, K. & Whitelaw, J. H.), pp. 5370. Springer.CrossRefGoogle Scholar
Antonia, R. A. & Kim, J. 1994 Low-Reynolds-number effects on near-wall turbulence. J. Fluid Mech. 276, 6180.CrossRefGoogle Scholar
Barri, M. & Andersson, H. I. 2010 Computer experiments on rapidly rotating plane Couette flow. Commun. Comput. Phys. 7, 683717.Google Scholar
Barri, M., El Khoury, G. K., Andersson, H. I. & Pettersen, B. 2009 Inflow conditions for inhomogeneous turbulent flows. Intl J. Numer. Meth. Fluids 60, 227235.CrossRefGoogle Scholar
Barri, M., El Khoury, G. K., Andersson, H. I. & Pettersen, B. 2010 DNS of backward-facing step flow with fully turbulent inflow. Intl J. Numer. Meth. Fluids 64, 777792.CrossRefGoogle Scholar
Beaudoin, J.-F., Cadot, O., Aider, J.-L. & Wesfreid, J. E. 2004 Three-dimensional stationary flow over a backward-facing step. Eur. J. Mech. B Fluids 23, 147155.CrossRefGoogle Scholar
Bech, K. H. & Andersson, H. I. 1997 Turbulent plane Couette flow subject to strong system rotation. J. Fluid Mech. 347, 289314.CrossRefGoogle Scholar
Bidokhti, A. A. & Tritton, D. J. 1992 The structure of a turbulent free shear layer in a rotating fluid. J. Fluid Mech. 241, 469502.CrossRefGoogle Scholar
Brethouwer, G. 2005 The effect of rotation on rapidly sheared homogeneous turbulence and passive scalar transport. Linear theory and direct numerical simulation. J. Fluid Mech. 542, 305342.CrossRefGoogle Scholar
Cambon, C., Benoit, J.-P., Shao, L. & Jacquin, L. 1994 Stability analysis and large-eddy simulation of rotating turbulence with organized eddies. J. Fluid Mech. 278, 175200.CrossRefGoogle Scholar
Cambon, C., Mansour, N. N. & Godeferd, F. S. 1997 Energy transfer in rotating turbulence. J. Fluid Mech. 337, 303332.CrossRefGoogle Scholar
Gartling, D. K. 1990 A test problem for outflow boundary conditions – flow over a backward-facing step. Intl J. Numer. Meth. Fluids 11, 953967.CrossRefGoogle Scholar
Grundestam, O., Wallin, S. & Johansson, A. V. 2008 Direct numerical simulation of rotating turbulent channel flow. J. Fluid Mech. 598, 177199.CrossRefGoogle Scholar
Hamman, C. W., Klewicki, J. C. & Kirby, R. M. 2008 On the Lamb vector divergence in Navier–Stokes flows. J. Fluid Mech. 610, 261284.CrossRefGoogle Scholar
Iida, O., Tsukamoto, Y. & Nagano, Y. 2008 The tilting mechanism of a longitudinal vortical structure in a homogenous shear flow with and without spanwise shear. Flow Turbul. Combust. 81, 1737.CrossRefGoogle Scholar
Johnston, J. P. 1998 Effects of system rotation on turbulence structure: a review relevant to turbomachinery flows. Intl J. Rotating Mach. 4, 97112.CrossRefGoogle Scholar
Johnston, J. P., Halleen, R. M. & Lezius, D. K. 1972 Effects of spanwise rotation on the structure of two-dimensional fully developed turbulent channel flow. J. Fluid Mech. 56, 533557.CrossRefGoogle Scholar
Kasagi, N. & Matsunaga, A. 1995 Three-dimensional particle-tracking velocimetry measurement of turbulent statistics and energy budget in a backward-facing step flow. Intl J. Heat Fluid Flow 16, 477485.CrossRefGoogle Scholar
Khaledi, H. A., Barri, M. & Andersson, H. I. 2009 On the stabilizing effect of the Coriolis force on the turbulent wake of a normal flat plate. Phys. Fluids 21, 095104.CrossRefGoogle Scholar
Kim, J., Moin, P. & Moser, R. 1987 Turbulence statistics in fully developed channel flow at low Reynolds number. J. Fluid Mech. 177, 133166.CrossRefGoogle Scholar
Klewicki, J. C. 1989 Velocity–vorticity correlations related to the gradients of the Reynolds stresses in parallel turbulent wall flows. Phys. Fluids A 1, 12851288.CrossRefGoogle Scholar
Kloosterziel, R. C. & van Heijst, G. J. F. 1991 An experimental study of unstable barotropic vortices in a rotating fluid. J. Fluid Mech. 223, 124.CrossRefGoogle Scholar
Kristoffersen, R. & Andersson, H. I. 1993 Direct simulations of low-Reynolds-number turbulent flow in a rotating channel. J. Fluid Mech. 256, 163197.CrossRefGoogle Scholar
Lamballais, E., Lesieur, M. & Métais, O. 1996 Effects of spanwise rotation on the vorticity stretching in transitional and turbulent channel flow. Intl J. Heat Fluid Flow 17, 324332.CrossRefGoogle Scholar
Lamballais, E., Métais, O. & Lesieur, M. 1998 Spectral-dynamic model for large-eddy simulations of turbulent rotating channel flow. Theor. Comput. Fluid Dyn. 12, 149177.CrossRefGoogle Scholar
Launder, B. E., Tselepidakis, D. P. & Younis, B. A. 1987 A second-moment closure study of rotating channel flow. J. Fluid Mech. 183, 6375.CrossRefGoogle Scholar
Le, H., Moin, P. & Kim, J. 1997 Direct numerical simulation of turbulent flow over a backward-facing step. J. Fluid Mech. 330, 349374.CrossRefGoogle Scholar
Liu, N.-S. & Lu, X.-Y. 2007 A numerical investigation of turbulent flows in a spanwise rotating channel. Comput. Fluids 36, 282298.CrossRefGoogle Scholar
Manhart, M. 2004 A zonal grid algorithm for DNS of turbulent boundary layers. Comput. Fluids 33, 435461.CrossRefGoogle Scholar
Meri, A. & Wengle, H. 2002 DNS and LES of turbulent backward-facing step flow using 2nd- and 4th-order discretization. In Advances in LES of Complex Flows (ed. Friedrich, R. & Rodi, W.), pp. 99114. Kluwer.CrossRefGoogle Scholar
Métais, O., Flores, C., Yanase, S., Riley, J. J. & Lesieur, M. 1995 Rotating free-shear flow. Part 2. Numerical simulations. J. Fluid Mech. 293, 4780.CrossRefGoogle Scholar
Nakabayashi, K. & Kitoh, O. 1996 Low Reynolds number fully developed two-dimensional turbulent channel flow with system rotation. J. Fluid Mech. 315, 129.CrossRefGoogle Scholar
Nakabayashi, K. & Kitoh, O. 2005 Turbulence characteristics of two-dimensional channel flow with system rotation. J. Fluid Mech. 528, 355377.CrossRefGoogle Scholar
Orlandi, P. 1997 Helicity fluctuations and turbulent energy production in rotating and non-rotating pipes. Phys. Fluids 9, 20452056.CrossRefGoogle Scholar
Orlanski, I. 1976 A simple boundary condition for unbounded hyperbolic flows. J. Comp. Physics 21, 251269.CrossRefGoogle Scholar
Rothe, P. H. & Johnston, J. P. 1979 Free shear layer behavior in rotating systems. J. Fluids Engng 101, 117120.CrossRefGoogle Scholar
Salhi, A. & Cambon, C. 1997 An analysis of rotating shear flow using linear theory and DNS and LES results. J. Fluid Mech. 347, 171195.CrossRefGoogle Scholar
Schäfer, F., Breuer, M. & Durst, F. 2009 The dynamics of the transitional flow over a backward-facing step. J. Fluid Mech. 623, 85119.CrossRefGoogle Scholar
Tennekes, H. & Lumley, J. L. 1972 A First Course in Turbulence. MIT Press.CrossRefGoogle Scholar
Tsinober, A. 1990 On one property of Lamb vector in isotropic turbulent flow. Phys. Fluids A 2, 484486.CrossRefGoogle Scholar
Yanase, S., Tanaka, M., Kida, S. & Kawahara, G. 2004 Generation and sustenance mechanisms of coherent vortical structures in rotating shear turbulence of zero-mean-absolute vorticity. Fluid Dyn. Res. 35, 237254.CrossRefGoogle Scholar

Barri and Andersson supplementary movie

Movie 1. Contour plots of instantaneous enstrophy fluctuations for Ro = 0.4. The contours are shown at the center of the channel. Dark contours indicate high energy regions.

Download Barri and Andersson supplementary movie(Video)
Video 18 MB

Barri and Andersson supplementary movie

Movie 1. Contour plots of instantaneous enstrophy fluctuations for Ro = 0.4. The contours are shown at the center of the channel. Dark contours indicate high energy regions.

Download Barri and Andersson supplementary movie(Video)
Video 16.6 MB

Barri and Andersson supplementary movie

Movie 2. Contour plots of instantaneous spanwise velocity fluctuations for Ro = 0.4 close to the stepped wall.

Download Barri and Andersson supplementary movie(Video)
Video 7.4 MB

Barri and Andersson supplementary movie

Movie 2. Contour plots of instantaneous spanwise velocity fluctuations for Ro = 0.4 close to the stepped wall.

Download Barri and Andersson supplementary movie(Video)
Video 7.1 MB

Barri and Andersson supplementary movie

Movie 3. Contour plots of instantaneous skin friction for Ro = 0.4. (a) at the straight upper-wall and (b) at the stepped lower-wall.

Download Barri and Andersson supplementary movie(Video)
Video 24.4 MB

Barri and Andersson supplementary movie

Movie 3. Contour plots of instantaneous skin friction for Ro = 0.4. (a) at the straight upper-wall and (b) at the stepped lower-wall.

Download Barri and Andersson supplementary movie(Video)
Video 8.5 MB