2011
DOI: 10.1080/10407782.2011.616843
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Effect of Channel-Confinement and Rotation on the Two-Dimensional Laminar Flow and Heat Transfer across a Cylinder

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Cited by 21 publications
(17 citation statements)
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“…7(a-e) shows the criss-cross motion of the shed-vortices, for eccentrically channel-confined flow across a stationary/rotating cylinder. This was proposed for stationary square cylinder by Suzuki et al (1993) and reported recently for rotating cylinder confined centrally in a channel by Prasad et al (2011). For stationary as well as rotating cylinder, the figure shows that the downstream distance at which the trajectory of positive and negative vortices cross each other increases with increasing eccentricity-ratio.…”
Section: Vorticity Contoursmentioning
confidence: 81%
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“…7(a-e) shows the criss-cross motion of the shed-vortices, for eccentrically channel-confined flow across a stationary/rotating cylinder. This was proposed for stationary square cylinder by Suzuki et al (1993) and reported recently for rotating cylinder confined centrally in a channel by Prasad et al (2011). For stationary as well as rotating cylinder, the figure shows that the downstream distance at which the trajectory of positive and negative vortices cross each other increases with increasing eccentricity-ratio.…”
Section: Vorticity Contoursmentioning
confidence: 81%
“…They further showed that the VS suppressed at higher Reynolds number ðRe Z Re c Þ. A more detailed study was reported, recently by Prasad et al (2011), at various rotationalvelocity ð0 r αr2Þ, blockage-ratio ð0% rβ r 50%Þ and Reynolds number ð35 r Re r170Þ. They found that the critical Reynolds number for the onset of VS increases, with increasing blockage ratio and increasing rotational velocity for stationary/rotating cylinder in a channel.…”
Section: Introductionmentioning
confidence: 86%
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