26th AIAA Applied Aerodynamics Conference 2008
DOI: 10.2514/6.2008-7344
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Discrete Structures in the Radial Flow Over a Rotor Blade in Dynamic Stall

Abstract: This paper confirms the finding of discrete quasi-periodic streamwise vortical structures in the radial flow behind the separation line over a rotor blade undergoing dynamic stall in forward flight. It follows our finding of such structures over a blade undergoing transient stall induced by an inflow obstructer in a hover facility. Co-rotating structures suggest that the free shear layer formed at stall rolls up into discrete cells. The spanwise spacing of structures is approximately the height of the separate… Show more

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Cited by 14 publications
(15 citation statements)
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“…17) suggest that the dynamic stall results are similar except near the blade tip, even though 3D stall (Ref. 18) exhibits the development of far more complex structures than two-dimensional (2D) stall (Ref. 19).…”
Section: Introductionmentioning
confidence: 88%
“…17) suggest that the dynamic stall results are similar except near the blade tip, even though 3D stall (Ref. 18) exhibits the development of far more complex structures than two-dimensional (2D) stall (Ref. 19).…”
Section: Introductionmentioning
confidence: 88%
“…When extended to airfoils and wings in dynamic regimes, Carta (1975) measured an additional non-uniform load distribution determined by these cellular flow structures, actively contributing to the presence of stall-delay. The presence of these stall-cell structures has been investigated as well in helicopter applications (Ottavio et al 2008). In these high aspect-ratio rotating-wings, the radial flow is the driver of the instability which brings to the development of cellular structures preventing the centrifugal increase of the radial-velocity distribution up to the tip.…”
Section: Loading Distributionmentioning
confidence: 99%
“…The pitch angle of the blade as a function of azimuth was manually set to follow the function θ(ψ) = θ o + θ c sinψ, where θ o is the collective pitch angle and θ c is the cyclic pitch angle. DiOttavio et al 21 please refer to DiOttavio et al 21 for more details on the kinematics of the experimental setup. Before and after each experimental run (total number of experimental runs = 102), the pitch angle was measured using a digital protractor at intervals of ψ = 30 • to verify the prescribed pitch angle variation with azimuth.…”
Section: A Experimental Setup and Flow Conditionsmentioning
confidence: 99%