1961
DOI: 10.1017/s0022112061000652
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Photographic evidence of the formation and growth of vorticity behind plates accelerated from rest in still air

Abstract: The shedding of vorticity from the edges of a plate, which is accelerated normal to itself from rest in still air, is investigated experimentally by means of a new flow-visualization technique using spark-lighted shadowgraphs and heated air, benzene or other vapours to introduce sufficient changes in density along the surface of discontinuity.The photographs show small-scale undulations and the formation of a number of centres of vorticity along the well known big-scale vortex sheets which roll up along their … Show more

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Cited by 81 publications
(27 citation statements)
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“…8 a and b. Similar small vortex structures were observed by Pierce (1961), and by Pullin and Perry (1980) who discussed whether these vortex like structures were really small vortices or the result of a vibrating system. As the tracers were introduced far upstream of these small vortices, the time history of the tracers due to disturbances made the visualized pictures difficult to analyze.…”
Section: The Second Stage: Generation Of Small Vorticessupporting
confidence: 71%
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“…8 a and b. Similar small vortex structures were observed by Pierce (1961), and by Pullin and Perry (1980) who discussed whether these vortex like structures were really small vortices or the result of a vibrating system. As the tracers were introduced far upstream of these small vortices, the time history of the tracers due to disturbances made the visualized pictures difficult to analyze.…”
Section: The Second Stage: Generation Of Small Vorticessupporting
confidence: 71%
“…These quantities were measured from the m o t i o n picture films. In order to correlate the test results of various model sizes a n d various flow accelerations, the measured results were " Pierce (1961) model (the width of the flat plate, the diameter of the circular disk or the diameter of the hollow hemi-sphere), a is the acceleration of the on-coming flow, t* is a characteristic time equal to the time that a fluid particle started from zero velocity travels a distance L/2 with constant acceleration a. The non-dimensional growth rate of the spiral starting vortex, ddv/df, and the translational speed of the spiral vortex center, d~v/df, are approximately constant during the starting stage, and are almost invariant for various model sizes and accelerations.…”
Section: Growth Of the Starting Vortexmentioning
confidence: 99%
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“…Nevertheless, in the same work, he proposed numerical solutions of regular and well defined start-up vortex spirals obtained by solving the Birkhoff-Rott equation written in similarity variables and without an explicit presence of the time variable. Moreover, the stability of this class of flows was not clarified by experiments that, performed by different authors, proposed different conclusions, Pierce [5], Pullin and Perry [6]. Luchini, among others, studied this phenomenon by computing the inviscid vortex shedding from a semi-infinite wedge [7] and from an airfoil [8].…”
Section: Introductionmentioning
confidence: 99%