Abstract
The instabilities in a sinusoidally oscillating non-separated flow over smooth circular
cylinders in the range of Keulegan–Carpenter numbers, K, from about 0.02 to 1
and Stokes numbers, β, from about 103 to 1.4 × 106 have been observed from
inception to chaos using several high-speed imagers and laser-induced fluorescence.
The instabilities ranged from small quasi-coherent structures, as in Stokes flow over
a flat wall (Sarpkaya 1993), to three-dimensional spanwise perturbations because
of the centrifugal forces induced by the curvature of the boundary layer (Taylor–Görtler
instability). These gave rise to streamwise-oriented counter-rotating vortices
or mushroom-shaped coherent structures as K approached the Kh values theoretically
predicted by Hall (1984). Further increases in K for a given β led first to complex
interactions between the coherent structures and then to chaotic motion. The mapping
of the observations led to the delineation of four states of flow in the (K, β)-plane:
stable, marginal, unstable, and chaotic.
Publisher
Cambridge University Press (CUP)
Subject
Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics
Cited by
52 articles.
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