2010
DOI: 10.1016/j.jfluidstructs.2010.02.001
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PIV measurement of separated flow over a blunt plate with different chord-to-thickness ratios

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Cited by 28 publications
(16 citation statements)
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“…The shortest plate in each branch (i.e., c/t¼3, 6 and 9) corresponded to regular vortex shedding, but increasing the c/t in each branch gave rise to irregularities in vortex shedding. Through particle image velocimetry (PIV) measurements of the flow at Re¼1 Â 10 3 , Shi et al (2010) convincingly demonstrated that the separated shear layer in a system with c/t¼ 3.0 did not re-attach to the plate's surface. Instead, the separated layer gave rise to a highly unstable wake, coupled with energetic leading-edge vortices.…”
Section: Introductionmentioning
confidence: 99%
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“…The shortest plate in each branch (i.e., c/t¼3, 6 and 9) corresponded to regular vortex shedding, but increasing the c/t in each branch gave rise to irregularities in vortex shedding. Through particle image velocimetry (PIV) measurements of the flow at Re¼1 Â 10 3 , Shi et al (2010) convincingly demonstrated that the separated shear layer in a system with c/t¼ 3.0 did not re-attach to the plate's surface. Instead, the separated layer gave rise to a highly unstable wake, coupled with energetic leading-edge vortices.…”
Section: Introductionmentioning
confidence: 99%
“…For a finite blunt plate in the presence of an undisturbed uniform free-stream flow, the Karman vortex street that would normally form behind a very short blunt plate can be considerably suppressed by elongating the plate in the streamwise direction. This elongation can produce entirely different vortex shedding features, depending on the chord-to-thickness ratio (Nakamura et al, 1991;Shi et al, 2010). However, in most practical situations, the flow is under considerable influence from the upstream turbulent flows, which are superimposed with the complex behavior of vortical structures.…”
Section: Introductionmentioning
confidence: 99%
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