Control of three-dimensional phase dynamics in a cylinder wake

Recently there has been a surge of new interest in three-dimensional wake patterns. In the present work, we have devised a method to control the spanwise end conditions and wake patterns using “end suction”, which is both continuously-variable and admits transient control. Classical steady-state patterns, such as parallel or oblique shedding or the “chevron” patterns are simply induced. The wake, at a given Reynolds number, is receptive to a continuous range of oblique shedding angles (θ), rather than to discrete angles, and there is excellent agreement with the “cos θ” formula for oblique-shedding frequencies. We show that the laminar shedding regime exists up to Reynolds numbers (Re) of 205, and that the immense disparity among reported critical Re for wake transition (Re = 140–190) can be explained in terms of spanwise end contamination. Our transient experiments have resulted in the discovery of new phenomena such as “phase shocks” and “phase expansions”, which can be explained in terms of a simple model assuming constant normal wavelength of the wake pattern. Peter Monkewitz (Lausanne) also predicts such transient phenomena from a Guinzburg-Landau model for the wake.

[1]  C. Williamson The natural and forced formation of spot-like ‘vortex dislocations’ in the transition of a wake , 1992, Journal of Fluid Mechanics.

[2]  M. Bloor,et al.  The transition to turbulence in the wake of a circular cylinder , 1964, Journal of Fluid Mechanics.

[3]  A. Roshko On the development of turbulent wakes from vortex streets , 1953 .

[4]  C. Williamson Defining a Universal and Continuous Strouhal-Reynolds Number Relationship for the Laminar Vortex She , 1988 .

[5]  Three-dimensional phase dynamics in a cylinder wake , 1994 .

[6]  Bernd R. Noack,et al.  Discrete Shedding Modes in the von Karman Vortex Street , 1993 .

[7]  Morteza Gharib,et al.  A novel method to promote parallel vortex shedding in the wake of circular cylinders , 1989 .

[8]  C. Williamson The Existence of Two Stages in the Transition to Three-Dimensionality of a Cylinder Wake , 1988 .

[9]  Description of transient states of von Kármán vortex streets by low‐dimensional differential equations , 1990 .

[10]  Boyer,et al.  Stability of vortex shedding modes in the wake of a ring at low Reynolds numbers. , 1993, Physical review letters.

[11]  D. Tritton Experiments on the flow past a circular cylinder at low Reynolds numbers , 1959, Journal of Fluid Mechanics.

[12]  G. Triantafyllou Three-Dimensional Flow Patterns in Two-Dimensional Wakes , 1992 .

[13]  Peter A. Monkewitz,et al.  A model for the formation of oblique shedding and ‘‘chevron’’ patterns in cylinder wakes , 1992 .

[14]  Bernd R. Noack,et al.  On cell formation in vortex streets , 1991 .

[15]  L. Redekopp,et al.  A model for pattern selection in wake flows , 1992 .

[16]  C. Williamson Oblique and parallel modes of vortex shedding in the wake of a circular cylinder at low Reynolds numbers , 1989, Journal of Fluid Mechanics.

[17]  C. Norberg An experimental investigation of the flow around a circular cylinder: influence of aspect ratio , 1994, Journal of Fluid Mechanics.

[18]  H. Eckelmann,et al.  The fine structure in the Strouhal-Reynolds number relationship of the laminar wake of a circular cylinder , 1990 .

[19]  Morteza Gharib,et al.  An experimental study of the parallel and oblique vortex shedding from circular cylinders , 1991, Journal of Fluid Mechanics.

[20]  Helmut Eckelmann,et al.  Vortex splitting and its consequences in the vortex street wake of cylinders at low Reynolds number , 1989 .