A note on bluff body vortex formation

Author:

Griffin Owen M.

Abstract

Green & Gerrard (1993) have presented in a recent paper the results of experiments to measure the distribution of vorticity in the near wake of a circular cylinder at low Reynolds numbers (up to Re = 220). They also compared the various definitions of the vortex formation region length which have been proposed by Gerrard (1966), Griffin (1974), and others for both high and low Reynolds numbers. The purpose of this note is to expand the work of Green & Gerrard, and to further their proposition that the end of the vortex formation region at all Reynolds numbers mark both the initial position of the fully shed vortex and the location at which its strength is a maximum. The agreement discussed here between several definitions for the formation region length will allow further understanding to be gained from investigations of the vortex wakes of stationary bluff bodies, and the wakes of oscillating bodies as well.

Publisher

Cambridge University Press (CUP)

Subject

Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics

Reference26 articles.

1. Griffin, O. M. & Votaw, C. W. 1972 The vortex street in the wake of a vibrating cylinder.J. Fluid Mech. 55,31–48.

2. Gerrard, J. H. 1966 The mechanics of the formation region of vortices behind bluff bodies.J. Fluid Mech. 25,401–413.

3. Griffin, O. M. & Ramberg, S. E. 1974 The vortex street wakes of vibrating cylinders.J. Fluid Mech. 66,553–576.

4. Griffin, O. M. 1971 The unsteady wake of an oscillating cylinder at low Reynolds number.Trans. ASME E:J. Appl. Mech. 38,729–738.

5. Griffin, O. M. 1974 Effects of synchronized cylinder vibration on vortex formation and mean flow.In Flow-Induced Structural Vibrations, IUTAM/IAHR Symposium Karlsruhe 1972 (ed. E. Naudascher ), pp.454–470.Springer.

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