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Excitation of shear layer instability in flow past a cylinder at low Reynolds number
Author(s) -
Mittal S.
Publication year - 2005
Publication title -
international journal for numerical methods in fluids
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.938
H-Index - 112
eISSN - 1097-0363
pISSN - 0271-2091
DOI - 10.1002/fld.1043
Subject(s) - wake , mechanics , reynolds number , instability , vortex shedding , physics , kármán vortex street , vortex , cylinder , shear flow , splitter plate , shear (geology) , classical mechanics , turbulence , materials science , geometry , mathematics , composite material
Abstract The instability of the separated shear layer for flow past a cylinder, in two dimensions, is investigated for low Reynolds numbers ( Re ⩽ 350). The line of symmetry, downstream of the cylinder, in the wake is forced to be a streamline. This hypothetical situation allows slip of velocity along the wake centreline but prevents any flow normal to it. With this arrangement the flow is completely stable for Re ⩽ 250. It suppresses the primary instability of the wake that is responsible for the von Karman vortex shedding. Unlike the conventional splitter plate such an arrangement does not have a wake of its own. At Re = 300 and above the wake instability and the shear layer instability are observed. The fluctuations due to the instabilities are intermittent in nature. The shear layer frequency is smaller than the frequency of the von Karman vortex shedding for the regular flow past a cylinder. It is also found that flow past half a cylinder, with symmetry conditions at the wake centreline, at Re = 300 is stable. However, when a secondary cylinder with one‐fifth the diameter of the half‐cylinder is placed close to it, the vortex shedding from the smaller cylinder again leads to instability of the separated shear layer of the half‐cylinder. This suggests that although the separated shear layer is stable, at such low Re , the shear layer instability can be excited by some other disturbances. It is found that even at such low Re , the normalized shear layer frequency follows the Re 0.67 power law. All the computations have been carried out using a stabilized finite element formulation. Copyright © 2005 John Wiley & Sons, Ltd.

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