2012
DOI: 10.1007/978-1-4614-3997-4_21
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Simulating Vortex Wakes of Flapping Plates

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Cited by 16 publications
(14 citation statements)
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“…A vortex-sheet model is efficient for slightly viscous flow because it can present the flow using vortex sheet, which is only one-dimensional in a 2D flow. It allows flow separations at prescribed locations (usually sharp edges), but it agrees quantitatively with Navier-Stokes models in predicting the strength of shed circulation, and the location of the primary vortices in the wake of an oscillated plate 31 . Previous work also shows a good agreement of the vortex-sheet model in predicting the stability boundary of a flapping flag 16 .…”
Section: Introductionmentioning
confidence: 71%
“…A vortex-sheet model is efficient for slightly viscous flow because it can present the flow using vortex sheet, which is only one-dimensional in a 2D flow. It allows flow separations at prescribed locations (usually sharp edges), but it agrees quantitatively with Navier-Stokes models in predicting the strength of shed circulation, and the location of the primary vortices in the wake of an oscillated plate 31 . Previous work also shows a good agreement of the vortex-sheet model in predicting the stability boundary of a flapping flag 16 .…”
Section: Introductionmentioning
confidence: 71%
“…In this model, vortex sheets approximate the thin viscous boundary layers along the body, which are advected from its trailing edge into the flow downstream. This can be regarded as the inviscid limit of the viscous flow, and gives a good representation of the large-scale features of the flow and the vortex wake dynamics at Reynolds numbers of O(10 2 -10 5 ) [31,39,40]. These flows are challenging to simulate directly due to the need to resolve sharp layers of vorticity in the vicinity of an unsteady, possibly deforming solid boundary.…”
Section: Introductionmentioning
confidence: 99%
“…The comprehension of this intermediate range of Reynolds numbers requires the correct modelling of the vortex dynamics detaching from the swimmer, and considerable efforts in this sense have been widely documented in the literature (see e.g. Michelin et al 2008;Alben 2009;Sheng et al 2012, and references therein). Lighthill (1960) and Wu (1961) established the theoretical foundation to understand reactive force production in a perfect fluid in, respectively, the slender-body limit and the two-dimensional limit.…”
Section: Introductionmentioning
confidence: 99%