1928
DOI: 10.1080/14786441108564677
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XCVI.The variation of velocity amplitude close to the surface of a cylinder moving through a viscous fluid

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Cited by 18 publications
(6 citation statements)
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“…Similar phenomena were detected in the next two investigations, one of circular cylinder flow (79) , the other of flow around a streamlined strut (80) . In the case of the cylinder (79) , the hot wire was also used to investigate separation around the cylinder's shoulder, the wire's signal being amplified so that the shed vorticity became audible (Fig. 25).…”
Section: The Aeronautical Departmentsupporting
confidence: 82%
“…Similar phenomena were detected in the next two investigations, one of circular cylinder flow (79) , the other of flow around a streamlined strut (80) . In the case of the cylinder (79) , the hot wire was also used to investigate separation around the cylinder's shoulder, the wire's signal being amplified so that the shed vorticity became audible (Fig. 25).…”
Section: The Aeronautical Departmentsupporting
confidence: 82%
“…Perhaps the eadiest indication that the flow in the stagnation region of a blunt body acquires a complex pattern is contained in two papers by Piercy & Richardson (1928, 1930, who concluded that "[there exists] a considerable area of instability extending upstream a distance about one-quarter of the length of the strut section and roughly covering the area for which the mean velocity is sensibly reduced below its value in the undisturbed stream .... Within the area explored, velocity amplitude (the amplitude of the usually observed fluctuating component) increases rapidly as the stagnation point is approached".…”
Section: Introductionmentioning
confidence: 99%
“…Widely known in the literature are the Görtler vortices generated at high Reynolds numbers in the boundary layer on a surface concave toward the freestream [1]. Experimental investigations of the incompressible transverse flow past a circular cylinder show that along the attachment line on the frontal surface of the body there appear vortex structures with a period equal to several boundary layer thicknesses [2]. At high Mach numbers M ∞ 1 the formation of spatially periodic vortices in the shock layer between the bow shock and the body surface is associated with considerable fluctuations of the enthalpy and heat flux distributions over the body surface.…”
mentioning
confidence: 99%