Loading…

Control of Dynamic Stall over a NACA 0015 Airfoil Using Plasma Actuators

Dynamic stall is observed in numerous applications, including sharply maneuvering fixed-wing aircraft, biomimetics, wind turbines, and most notably, rotorcraft. The associated unsteady loading can lead to aerodynamic flutter and mechanical failure in the system. The present work explores the ability...

Full description

Saved in:
Bibliographic Details
Published in:AIAA journal 2018-01, Vol.56 (1), p.78-89
Main Authors: Singhal, Achal, Castañeda, David, Webb, Nathan, Samimy, Mo
Format: Article
Language:English
Subjects:
Citations: Items that this one cites
Items that cite this one
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
Description
Summary:Dynamic stall is observed in numerous applications, including sharply maneuvering fixed-wing aircraft, biomimetics, wind turbines, and most notably, rotorcraft. The associated unsteady loading can lead to aerodynamic flutter and mechanical failure in the system. The present work explores the ability of nanosecond pulse-driven dielectric barrier discharge plasma actuators to control dynamic stall over a NACA 0015 airfoil. The Reynolds number, reduced frequency, and excitation Strouhal number were varied over large ranges: Re=167,000–500,000, k=0.025–0.075, and Ste=0–10, respectively. Surface pressure measurements were taken for each combination of Reynolds number, reduced frequency, and excitation Strouhal number. Phase-locked particle image velocimetry measurements were acquired for select cases. It was observed that the trends of effect of Ste were similar for all combinations of Reynolds number and reduced frequency, and three major conclusions were drawn. First, it was observed that low Strouhal number excitation (Ste2. Second, all excitation resulted in earlier flow reattachment. Last, it was shown that excitation, especially at high Ste, resulted in reduced aerodynamic hysteresis and dynamic stall vortex strength. The decrease in the strength of the dynamic stall vortex is achieved by the formation of large-scale structures induced by the excitation that bleed the leading-edge vorticity before the ejection of the dynamic stall vortex. At sufficiently high excitation Strouhal numbers (Ste≈10), the dynamic stall vortex was completely suppressed.
ISSN:0001-1452
1533-385X
DOI:10.2514/1.J056071