Abstract

In the present study, an oscillating membrane flapper was pivotally attached to the tip of a conventional rigid wing. Stroke-averaged aerodynamic forces were measured for the range of the flapping frequency, showing significant increases in the lift coefficient and lift-to-drag ratio for the wing with a flapper. Major vortex patterns were deduced from observations of smoke-wire visualization and 2D phase-locked particle image velocimetry (PIV). The centerline of the primary vortex wanders in the counterclockwise direction. On the contrary, its core rotates in the same sense of rotation as a wingtip vortex in a conventional wing. The secondary weaker vortex of opposite rotation lasts for a half stroke. The vortex ring sheds from the flapper during the second half of the upstroke and pronation. The outer parts of the vortex system are much stronger than the inner ones. The circulation and size of vortices decrease significantly at the most distant station from the wing. Strong vertical jets were found in smoke-wire visualization and confirmed with velocity and vorticity fields obtained by PIV. These jets are formed between undulating vortices and inside of the vortex ring. The jet airflow moves away from the flapper and downward or upward depending on the flapping direction.

Highlights

  • The airflow around a conventional wing features wingtip vortices produced by spanwise flows and a pressure differential over the top and bottom surfaces of the wing

  • The vortex core rotates in a clockwise direction (Figure 12), which is the same sense of rotation as a wingtip vortex in a conventional fixed wing

  • Stroke-averaged aerodynamic forces were measured in the wing with a wingtip flapper for the range of flapping frequency 20–30 Hz

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Summary

Introduction

The airflow around a conventional wing features wingtip vortices produced by spanwise flows and a pressure differential over the top and bottom surfaces of the wing. A proximity of a wingtip changes a pressure distribution over the wing surface resulting in the induced drag. Wingtip vortices roll up over the wing edge, shed, and dissipate downstream. They may persist along the flight path, creating a safety hazard to other aircraft. Effects of wingtip configurations on wing aerodynamics have been investigated by many authors. Sohn and Chang [1] compared a simple wingtip fairing to Whitcomb’s winglet design [2]

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