Three-Dimensional Effects on Sliding and Waving Wings
Like large insects, micro air vehicles operate at low Reynolds numbers O(1; 000-10; 000) in a regime characterized by separated flow and strong vortices. The leading-edge vortex has been identified as a significant source of high lift on insect wings, but the conditions required for the formation of...
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Veröffentlicht in: | Journal of aircraft 2011-03, Vol.48 (2), p.633-644 |
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Sprache: | eng |
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Zusammenfassung: | Like large insects, micro air vehicles operate at low Reynolds numbers O(1; 000-10; 000) in a regime characterized by separated flow and strong vortices. The leading-edge vortex has been identified as a significant source of high lift on insect wings, but the conditions required for the formation of a stably attached leading-edge vortex are not yet known. The waving wing is designed to model the translational phase of an insect wing stroke by preserving the unsteady starting and stopping motion as well as three-dimensionality in both wing geometry (via a finite-span wing) and kinematics (via wing rotation). The current study examines the effect of the spanwise velocity gradient on the development of the leading-edge vortex along the wing as well as the effects of increasing three-dimensionality by decreasing wing aspect ratio from four to two. Dye flow visualization and particle image velocimetry reveal that the leading-edge vortices that form on a sliding or waving wing have a very high aspect ratio. The structure of the flow is largely two-dimensional on both sliding and waving wings and there is minimal interaction between the leading-edge vortices and the tip vortex. Significant spanwise flow was observed on the waving wing but not on the sliding wing. Despite the increased three-dimensionality on the aspect ratio 2 waving wing, there is no evidence of an attached leading-edge vortex and the structure of the flow is very similar to that on the higher-aspect-ratio wing and sliding wing. [PUBLICATION ABSTRACT] |
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ISSN: | 0021-8669 1533-3868 |
DOI: | 10.2514/1.C031184 |