Flow Control over a Nonslender Delta Wing by Microsecond Dielectric Barrier Discharge Actuation

The behaviors of a pulsed microsecond dielectric barrier discharge in quiescent air are diagnosed by schlieren image and particle image velocimetry. Some localized pressure waves are induced by the discharge, propagating at a speed of about 348.5  m/s. A fairly weak vortex is also induced, with a ma...

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Veröffentlicht in:AIAA journal 2020-01, Vol.58 (1), p.61-70
Hauptverfasser: Zhao, Guangyin, Liang, Hua, Niu, Zhongguo
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Liang, Hua
Niu, Zhongguo
description The behaviors of a pulsed microsecond dielectric barrier discharge in quiescent air are diagnosed by schlieren image and particle image velocimetry. Some localized pressure waves are induced by the discharge, propagating at a speed of about 348.5  m/s. A fairly weak vortex is also induced, with a maximum velocity of about 0.1  m/s. Wind tunnel experiments are conducted on a wing–body combination with a 47 deg swept wing. Three actuator arrangements are tested by force measurements. For the full leading-edge actuation, obvious changes of the normal forces can be achieved at high angles of attack before stall, when the actuator works at the optimum reduced frequency of F+≈1–2. However, the stall angle is not delayed under the actuation. For front-half actuation at the leading edge, the obvious control effect is obtained at large angles of attack (22–30 deg), while for rear-half actuation, the normal force gets a relatively modest increase at a broad range of attack angles (10–34 deg). The flow pattern obtained by particle image velocimetry shows that the actuation frequency mainly determines the number of chordwise vortices coexisting along the shear layer. It is hard to engender the reattachment vortex over the wing under high-frequency actuations (such as F+=4).
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Some localized pressure waves are induced by the discharge, propagating at a speed of about 348.5  m/s. A fairly weak vortex is also induced, with a maximum velocity of about 0.1  m/s. Wind tunnel experiments are conducted on a wing–body combination with a 47 deg swept wing. Three actuator arrangements are tested by force measurements. For the full leading-edge actuation, obvious changes of the normal forces can be achieved at high angles of attack before stall, when the actuator works at the optimum reduced frequency of F+≈1–2. However, the stall angle is not delayed under the actuation. For front-half actuation at the leading edge, the obvious control effect is obtained at large angles of attack (22–30 deg), while for rear-half actuation, the normal force gets a relatively modest increase at a broad range of attack angles (10–34 deg). The flow pattern obtained by particle image velocimetry shows that the actuation frequency mainly determines the number of chordwise vortices coexisting along the shear layer. 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See also AIAA Rights and Permissions .</rights><rights>Copyright © 2019 by the American Institute of Aeronautics and Astronautics, Inc. All rights reserved. All requests for copying and permission to reprint should be submitted to CCC at www.copyright.com; employ the eISSN 1533-385X to initiate your request. 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Some localized pressure waves are induced by the discharge, propagating at a speed of about 348.5  m/s. A fairly weak vortex is also induced, with a maximum velocity of about 0.1  m/s. Wind tunnel experiments are conducted on a wing–body combination with a 47 deg swept wing. Three actuator arrangements are tested by force measurements. For the full leading-edge actuation, obvious changes of the normal forces can be achieved at high angles of attack before stall, when the actuator works at the optimum reduced frequency of F+≈1–2. However, the stall angle is not delayed under the actuation. For front-half actuation at the leading edge, the obvious control effect is obtained at large angles of attack (22–30 deg), while for rear-half actuation, the normal force gets a relatively modest increase at a broad range of attack angles (10–34 deg). The flow pattern obtained by particle image velocimetry shows that the actuation frequency mainly determines the number of chordwise vortices coexisting along the shear layer. 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The flow pattern obtained by particle image velocimetry shows that the actuation frequency mainly determines the number of chordwise vortices coexisting along the shear layer. It is hard to engender the reattachment vortex over the wing under high-frequency actuations (such as F+=4).</abstract><cop>Virginia</cop><pub>American Institute of Aeronautics and Astronautics</pub><doi>10.2514/1.J058649</doi><tpages>10</tpages></addata></record>
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subjects Actuation
Actuators
Aerodynamics
Angle of attack
Delta wings
Dielectric barrier discharge
Elastic waves
Flow control
Flow pattern
Fluid dynamics
Fluid flow
Force measurement
Particle image velocimetry
Plasma
Shear layers
Swept wings
Wave propagation
Wind tunnel testing
Wind tunnels
title Flow Control over a Nonslender Delta Wing by Microsecond Dielectric Barrier Discharge Actuation
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