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Instability of flow around a rotating, semi-infinite cylinder

Srikanth Derebail Muralidhar, Benoît Pier, and Julian F. Scott

  • Laboratoire de mécanique des fluides et d'acoustique, CNRS–École centrale de Lyon–Université de Lyon 1–INSA Lyon, 36 avenue Guy-de-Collongue, 69134 Écully, France

Phys. Rev. Fluids 1, 053602 – Published 16 September, 2016

DOI: https://doi.org/10.1103/PhysRevFluids.1.053602

Abstract

Stability of flow around a rotating, semi-infinite cylinder placed in an axial stream is investigated. Assuming large Reynolds number, the basic flow is computed numerically as described by Derebail Muralidhar et al. [Proc. R. Soc. London, Ser. A 472, 20150850 (2016)], while numerical solution of the local stability equations allows calculation of the modal growth rates and hence determination of flow stability or instability. The problem has three nondimensional parameters: the Reynolds number Re, the rotation rate S, and the axial location Z. Small amounts of rotation are found to strongly affect flow stability. This is the result of a nearly neutral mode of the nonrotating cylinder which controls stability at small S. Even small rotation can produce a sufficient perturbation that the mode goes from decaying to growing, with obvious consequences for stability. Without rotation, the flow is stable below a Reynolds number of about 1060 and also beyond a threshold Z. With rotation, no matter how small, instability is no longer constrained by a minimum Re nor a maximum Z. In particular, the critical Reynolds number goes to zero as Z, so the flow is always unstable at large enough axial distances from the nose. As Z is increased, the flow goes from stability at small Z to instability at large Z. If the critical Reynolds number is a monotonic decreasing function of Z, as it is for S between about 0.0045 and 5, there is a single boundary in Z, which separates the stable from the unstable part of the flow. On the other hand, when the critical Reynolds number is nonmonotonic, there can, depending on the choice of Re, be several such boundaries and flow stability switches more than once as Z is increased. Detailed results showing the critical Reynolds number as a function of Z for different rotation rates are given. We also obtain an asymptotic expansion of the critical Reynolds number at large Z and use perturbation theory to further quantify the behavior at small S.

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References (21)

  1. H. L. Reed and W. S. Saric, Stability of three-dimensional boundary layers, Annu. Rev. Fluid Mech. 21, 235 (1989).
  2. W. S. Saric, H. L. Reed, and E. B. White, Stability and transition of three-dimensional boundary layers, Annu. Rev. Fluid Mech. 35, 413 (2003).
  3. R. J. Lingwood, Absolute instability of the boundary layer on a rotating disk, J. Fluid Mech. 299, 17 (1995).
  4. B. Pier, Primary crossflow vortices, secondary absolute instabilities and their control in the rotating-disk boundary layer, J. Eng. Math. 57, 237 (2007).
  5. S. J. Garrett and N. Peake, The absolute instability of the boundary layer on a rotating cone, Eur. J. Mech. B: Fluids 26, 344 (2007).
  6. S. J. Garrett, Z. Hussain, and S. O. Stephen, Boundary-layer transition on broad cones rotating in an imposed axial flow, AIAA J. 48, 1184 (2010).
  7. B. Pier, Periodic and quasiperiodic vortex shedding in the wake of a rotating sphere, J. Fluids Struct. 41, 43 (2013).
  8. S. Derebail Muralidhar, B. Pier, J. F. Scott, and R. Govindarajan, Flow around a rotating, semi-infinite cylinder in an axial stream, Proc. R. Soc. London, Ser. A 472, 20150850 (2016).
  9. W. Tollmien, Über die Entstehung der Turbulenz. 1. Mitteilung, Nachr. Ges. Wiss. Goettingen, Math. Phys. Kl. 1929, 21 (1928).
  10. R. Jordinson, The flat plate boundary layer. Part 1. Numerical integration of the Orr-Sommerfeld equation, J. Fluid Mech. 43, 801 (1970).
  11. L. M. Mack, A numerical study of the temporal eigenvalue spectrum of the Blasius boundary layer, J. Fluid Mech. 73, 497 (1976).
  12. O. R. Tutty, W. G. Price, and A. T. Parsons, Boundary layer flow on a long thin cylinder, Phys. Fluids 14, 628 (2002).
  13. N. Vinod and R. Govindarajan, Secondary instabilities in incompressible axisymmetric boundary layers: Effect of transverse curvature, J. Fluids Eng. 134, 024503 (2012).
  14. K. H. Kao and C. Y. Chow, Stability of the boundary layer on a spinning semi-infinite circular cylinder, J. Spacecr. Rockets 28, 284 (1991).
  15. M. A. Herrada, C. Del Pino, and R. Fernandez-Feria, Stability of the boundary layer flow on a long thin rotating cylinder, Phys. Fluids 20, 034105 (2008).
  16. J. T. Kegelman, R. C. Nelson, and T. J. Mueller, The boundary layer on an axisymmetric body with and without spin, AIAA J. 21, 1485 (1983).
  17. M. G. Hall, Vortex breakdown, Annu. Rev. Fluid Mech. 4, 195 (1972).
  18. C. Leclercq, Instabilités convectives et absolues dans l'écoulement de Taylor-Couette-Poiseuille excentrique, Ph.D. thesis, École centrale de Lyon, 2013.
  19. P. J. Schmid and D. S. Henningson, Stability and Transition in Shear Flows, Applied Mathematical Sciences (Springer, New York, 2001).
  20. L. N. Howard and A. S. Gupta, On the hydrodynamic and hydromagnetic stability of swirling flows, J. Fluid Mech. 14, 463 (1962).
  21. T. J. Pedley, On the instability of viscous flow in a rapidly rotating pipe, J. Fluid Mech. 35, 97 (1969).

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