Hostname: page-component-586b7cd67f-r5fsc Total loading time: 0 Render date: 2024-11-24T19:36:31.207Z Has data issue: false hasContentIssue false

Laminar to fully turbulent flow in a pipe: scalar patches, structural duality of turbulent spots and transitional overshoot

Published online by Cambridge University Press:  28 May 2020

Xiaohua Wu
Affiliation:
Department of Mechanical and Aerospace Engineering, Royal Military College of Canada, Kingston, ONK7K 7B4, Canada
Parviz Moin*
Affiliation:
Center for Turbulence Research, Stanford University, Stanford, CA94305-3035, USA
Ronald J. Adrian
Affiliation:
School for the Engineering of Matter, Transport and Energy, Arizona State University, Tempe,AZ85287-6106, USA
*
Email address for correspondence: [email protected]

Abstract

We present findings on scalar flashes, turbulent spots and transition statistics in a direct numerical simulation of a 500 radius-long pipe flow with a radial-mode inlet disturbance. Transitional spots are found to contain two different types of eddies. The wall region consists primarily of ‘reverse hairpin vortices’. This unusual structure is related to the high-speed streaks arising from the prescribed inlet perturbation. The core region is populated by the normally observed ‘forward’ hairpin vortices. Number density of the reverse hairpins is quantified indirectly and conservatively by measuring the number density of negative skin-friction patches. During the late stages of transition, second-order statistics such as Reynolds stresses and the rate of dissipation of turbulent kinetic energy exhibit substantial overshoot. This is associated with mid-to-high frequency content in the energy spectra that exceeds the corresponding levels in fully developed turbulence. Flow visualizations reveal bursts of small-scale vortex motions, including the reverse hairpins, that probably account for the enhanced mid-to-high frequency spectral content. A passive scalar is injected at the centreline of the inlet plane, mimicking laboratory injection of dye through a needle, to investigate the mysterious phenomenon of turbulent scalar patches residing in fully developed turbulent pipe flow. At several hundred radii downstream of transition where the velocity field is genuine fully developed turbulence, the scalar patches retain persistent memory of events far upstream. Comparing the present flow with a similar pipe flow disturbed by a significantly different inlet condition suggests that the foregoing observations are insensitive to the form of the disturbances.

Type
JFM Papers
Copyright
© The Author(s), 2020. Published by Cambridge University Press

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

Acarlar, M. M. & Smith, C. R. 1987 A study of hairpin vortices in a laminar boundary layer. Part 2. Hairpin vortices generated by fluid injection. J. Fluid Mech. 175, 4383.CrossRefGoogle Scholar
Adrian, R. J. 2007 Hairpin vortex organization in wall turbulence. Phys. Fluids 19, 041301.CrossRefGoogle Scholar
Adrian, R. J., Meinhart, C. D. & Tomkins, C. D. 2000 Vortex organization in the turbulent boundary layer. J. Fluid Mech. 422, 154.CrossRefGoogle Scholar
Avila, K., Moxey, D., de LOZAR, A., Avila, M., Barkley, D. & Hof, B. 2011 The onset of turbulence in pipe flow. Science 333, 192196.CrossRefGoogle ScholarPubMed
Bandyopadhyay, P. R. 1986 Aspects of the equilibrium puff in transitional pipe flow. J. Fluid Mech. 163, 439458.CrossRefGoogle Scholar
Barkley, D., Song, B., Mukund, V., Lemoult, G., Avila, M. & Hof, B. 2015 The rise of fully turbulent flow. Nature 526, 550553.CrossRefGoogle ScholarPubMed
Cardesa, J. I., Monty, J. P., Soria, J. & Chong, M. S. 2019 The structure and dynamics of backflow in turbulent channels. J. Fluid Mech. 880, R3.CrossRefGoogle Scholar
Chin, C., Ooi, A. S. H., Marusic, I. & Blackburn, H. M. 2010 The influence of pipe length on turbulence statistics computed from direct numerical simulation data. Phys. Fluids 22, 115107.CrossRefGoogle Scholar
Chin, R. C., Monty, J. P., Chong, M. S. & Marusic, I. 2018 Conditionally averaged flow topology about a critical point pair in skin-friction field of pipe flows using direct numerical simulations. Phys. Rev. Fluids 3, 114607.CrossRefGoogle Scholar
Choi, H. & Moin, P. 1990 On the space–time characteristics of wall-pressure fluctuations. Phys. Fluids A 2, 14501460.CrossRefGoogle Scholar
Duguet, Y., Willis, A. P. & Kerswell, R. R. 2010 Slug genesis in cylindrical pipe flow. J. Fluid Mech. 663, 180208.CrossRefGoogle Scholar
Eckhardt, B., Schneider, T. M., Hof, B. & Westerweel, J. 2007 Turbulence transition in pipe flow. Annu. Rev. Fluid Mech. 39, 447468.CrossRefGoogle Scholar
Erm, L. P. & Joubert, P. N. 1991 Low-Reynolds-number turbulent boundary layers. J. Fluid Mech. 230, 144.CrossRefGoogle Scholar
Goto, S., Kida, S. & Fujiwara, S. 2011 Flow visualization using reflective flakes. J. Fluid Mech. 683, 417429.CrossRefGoogle Scholar
Herbert, T. 1988 Secondary instability of boundary layers. Annu. Rev. Fluid Mech. 20, 487526.CrossRefGoogle Scholar
Jalalabadi, R. & Sung, H. J. 2018 Influence of backflow on skin friction in turbulent pipe flow. Phys. Fluids 30, 065104.CrossRefGoogle Scholar
Leonard, A.1983 Numerical simulation of turbulent flows. NACA TM 84320.Google Scholar
Lindgren, E. R. 1953 Some aspects of the change between laminar and turbulent flow of liquids in cylindrical tubes. Arkiv. Fys. 3, 293308.Google Scholar
Lindgren, E. R. 1959a Liquid flow in tubes I. The transition process under highly disturbed entrance flow conditions. Arkiv. Fys. 15, 97119.Google Scholar
Lindgren, E. R. 1959b Liquid flow in tubes II. The transition process under less disturbed inlet flow conditions. Arkiv. Fys. 15, 503519.Google Scholar
Lindgren, E. R. 1959c Liquid flow in tubes III. Characteristic data of the transition process. Arkiv. Fys. 16, 101112.Google Scholar
Moin, P. & Kim, J. 1985 The structure of the vorticity field in turbulent channel flow. Part 1. Analysis of instantaneous fields and statistical correlations. J. Fluid Mech. 608, 81112.Google Scholar
Moxey, D. & Barkley, D. 2010 Distinct large-scale turbulent-laminar states in transitional pipe flow. Proc. Natl Acad. Sci USA 107, 80918096.CrossRefGoogle ScholarPubMed
Mullin, T. 2011 Experimental studies of transition to turbulence in a pipe. Annu. Rev. Fluid Mech. 43, 124.CrossRefGoogle Scholar
Peixinho, J. & Mullin, T. 2007 Finite-amplitude thresholds for transition in pipe flow. J. Fluid Mech. 582, 169178.CrossRefGoogle Scholar
Pierce, C. D. & Moin, P.2001 Progress variable approach for large-eddy simulation of turbulent combustion. Mech. Eng. Dept. Rep. TF-80, Stanford University.Google Scholar
Pierce, C. D. & Moin, P. 2004 Progress variable approach for large-eddy simulation of non-premixed turbulent combustion. J. Fluid Mech. 504, 7397.CrossRefGoogle Scholar
Priymak, V. G. & Miyazaki, T. 2004 Direct numerical simulation of equilibrium spatially localized structures in pipe flow. Phys. Fluids 16, 42214234.CrossRefGoogle Scholar
Purtell, L. P., Klebanoff, P. S. & Buckley, F. T. 1981 Turbulent boundary layer at low Reynolds number. Phys. Fluids 24, 802811.CrossRefGoogle Scholar
Reynolds, O. 1883 An experimental investigation of the circumstances which determine whether the motion of water shall be direct or sinuous, and of the law of resistance in parallel channels. Phil. Trans. R. Soc. Lond. A 174, 935982.Google Scholar
Rogers, M. M. & Moin, P. 1987 The structure of the vorticity field in homogeneous turbulent flows. J. Fluid Mech. 176, 3366.CrossRefGoogle Scholar
Sau, R. & Mahesh, K. 2008 Dynamics and mixing of vortex rings in crossflow. J. Fluid Mech. 604, 389409.CrossRefGoogle Scholar
Sayadi, T., Hamman, C. W. & Moin, P. 2013 Direct numerical simulation of complete H-type and K-type transitions with implications for the dynamics of turbulent boundary layers. J. Fluid Mech. 724, 480509.CrossRefGoogle Scholar
Schubauer, G. B. & Klebanoff, P. S.1955 Contributions on the mechanics of boundary layer transition. NACA Tech. Note 3489.Google Scholar
Schubauer, G. B. & Skramstad, H. K. 1947 Laminar boundary-layer oscillations and stability of laminar flow. J. Aero. Sci. 14, 8897.CrossRefGoogle Scholar
Shan, H., Ma, B., Zhang, Z. & Nieuwstadt, F. T. M. 1999 Direct numerical simulation of a puff and a slug in transitional cylindrical pipe flow. J. Fluid Mech. 387, 3960.CrossRefGoogle Scholar
Shimizu, M. & Kida, S. 2009 A driving mechanism of a turbulent puff in pipe flow. Fluid Dyn. Res. 41, 045501.CrossRefGoogle Scholar
Vanderwel, C. & Tavoularis, S. 2011 Coherent structures in uniformly sheared turbulent flow. J. Fluid Mech. 689, 434464.CrossRefGoogle Scholar
Wallace, J. M. 2016 Quadrant analysis in turbulence research: history and evolution. Annu. Rev. Fluid Mech. 48, 131158.CrossRefGoogle Scholar
Willis, A. P. & Kerswell, R. R. 2007 Critical behavior in the re-laminarization of localized turbulence in pipe flow. Phys. Rev. Lett. 98, 014501.CrossRefGoogle ScholarPubMed
Winters, K. J. & Longmire, E. K. 2019 PIV-based characterization of puffs in transitional pipe flow. Exp. Fluids 60, 60.CrossRefGoogle Scholar
Wu, X. 2017 Inflow turbulence generation methods. Annu. Rev. Fluid Mech. 49, 2349.CrossRefGoogle Scholar
Wu, X., Cruickshank, M. & Ghaemi, S. 2020 Negative skin-friction during transition in zero-pressure-gradient flat-plate boundary layer and in pipe flows with the slip and no-slip boundary conditions. J. Fluid Mech. 887, A26.CrossRefGoogle Scholar
Wu, X., Jacobs, R. G., Hunt, J. C. R. & Durbin, P. A. 1999 Simulation of boundary layer transition induced by periodically passing wakes. J. Fluid Mech. 398, 109153.CrossRefGoogle Scholar
Wu, X. & Moin, P. 2008 A direct numerical simulation study on the mean velocity characteristics in turbulent pipe flow. J. Fluid Mech. 608, 81112.CrossRefGoogle Scholar
Wu, X. & Moin, P. 2009 Direct numerical simulation of turbulence in a nominally zero-pressure-gradient flat-plate boundary layer. J. Fluid Mech. 630, 541.CrossRefGoogle Scholar
Wu, X. & Moin, P. 2010 Transitional and turbulent boundary layer with heat transfer. Phys. Fluids 22, 85105.CrossRefGoogle Scholar
Wu, X., Moin, P., Adrian, R. J. & Baltzer, J. R. 2015 Osborne Reynolds pipe flow: direct simulation from laminar through gradual transition to fully developed turbulence. Proc. Natl Acad. Sci. USA 112, 79207924.CrossRefGoogle ScholarPubMed
Wu, X., Moin, P., Wallace, J. M., Skarda, J., Adrián, L.-D. & Hickey, J.-P. 2017 Transitional-turbulent spots and turbulent–turbulent spots in boundary layers. Proc. Natl Acad. Sci. USA 114, E5292E5299.CrossRefGoogle ScholarPubMed
Wygnanski, I. J. & Champagne, F. H. 1973 On transition in a pipe. Part 1. The origin of puffs and slugs and the flow in a turbulent slug. J. Fluid Mech. 59, 281335.CrossRefGoogle Scholar
Zheng, W., Yang, Y. & Chen, S. 2016 Evolutionary geometry of Lagrangian structures in a transitional boundary layer. Phys. Fluids 28, 035110.CrossRefGoogle Scholar
Zhou, J., Adrian, R. J., Balachandar, S. & Kendall, T. M. 1999 Mechanisms for generating coherent packets of hairpin vortices in channel flow. J. Fluid Mech. 387, 353396.CrossRefGoogle Scholar