1991
DOI: 10.1016/0045-7930(91)90034-f
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On steady flow past a rotating circular cylinder at Reynolds numbers 60 and 100

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Cited by 80 publications
(38 citation statements)
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“…It is also noticed that this separation bubble tilts upwards and sits on the shoulder of the cylinder. Similar asymmetrical streamline pattern due to rotation are also reported in [34,35]. A picture with vanishing lower bubble is given in [35] at the Reynolds number of 60 and q = 1.…”
Section: Tip Velocity Ratio Q = 20supporting
confidence: 59%
“…It is also noticed that this separation bubble tilts upwards and sits on the shoulder of the cylinder. Similar asymmetrical streamline pattern due to rotation are also reported in [34,35]. A picture with vanishing lower bubble is given in [35] at the Reynolds number of 60 and q = 1.…”
Section: Tip Velocity Ratio Q = 20supporting
confidence: 59%
“…In this representation, the far-ÿeld boundary condition that the ow remains undisturbed needs to be carefully dealt with during numerical implementation [16].…”
Section: Introductionmentioning
confidence: 99%
“…The degree of rotation is often quantified by the nondimensional rotation rate, α = ωd/(2U ), defined as the ratio of the tangential surface speed (ωd/2, with ω the angular velocity) and the free-stream speed U . Many authors, including Tang & Ingham (1991), have shown that imposing a rotation on the body renders the wake asymmetrical and, at Re 60, depending on the rotation rate, the elimination of one or both of the recirculation regions in the wake can be observed. For larger Re, the imposed rotation may also suppress or delay the transition to unsteady flow in comparison to the case of a non-rotating body.…”
Section: Introductionmentioning
confidence: 99%