Plasma Volumetric Effects on the Force Production of a Plasma Actuator

Dielectric barrier discharge plasma actuators are examined experimentally and computationally. Experimental temporal force measurements show that the plasma actuator produces two positive (accelerating) forces per ac cycle. While the plasma is ignited, the actuator experiences an accelerating force, and, when the plasma is extinguished, a decelerating force appears. This occurs twice during each ac bias cycle. In addition, while the accelerating force is approximately equal in magnitude and direction during each half of the ac cycle, the decelerating force is not. Navier― Stokes simulations of the neutral air flow with a prescribed plasma force reveal that the variation in the decelerating actuator force is consistent with structural changes in the plasma itself. These plasma structural changes alter the volume over which the plasma force is imparted to the air and, in turn, change the amount of air drag incurred by the wall jet created by the plasma. During each actuator bias cycle, 70―90% of the momentum supplied by the plasma actuator is destroyed by drag with the wall immediately after the plasma extinguishes.

[1]  Thomas McLaughlin,et al.  Time-correlated force production measurements of the dielectric barrier discharge plasma aerodynamic actuator , 2008 .

[2]  M. Kotsonis,et al.  Numerical Study on Control of Tollmien-Schlichting Waves Using Plasma Actuators , 2011 .

[3]  E. Moreau,et al.  Optimization of a dielectric barrier discharge actuator by stationary and non-stationary measurements of the induced flow velocity: application to airflow control , 2007 .

[4]  Gabriel Font,et al.  Plasma Discharges in Atmospheric Pressure Oxygen for Boundary Layer Separation Control , 2005 .

[5]  J. Murthy,et al.  A PRESSURE-BASED METHOD FOR UNSTRUCTURED MESHES , 1997 .

[6]  Leanne Pitchford,et al.  Model description of surface dielectric barrier discharges for flow control , 2008 .

[7]  L. C. Pitchford,et al.  Electrohydrodynamic force in dielectric barrier discharge plasma actuators , 2007 .

[8]  D. M. Orlov,et al.  Characterization of Discharge Modes of Plasma Actuators , 2008 .

[9]  T. McLaughlin,et al.  Effects of Oxygen Content on Dielectric Barrier Discharge Plasma Actuator Behavior , 2011 .

[10]  Sanjay R. Mathur,et al.  A Reynolds-averaged Navier-Stokes solver using unstructured mesh-based finite-volume scheme , 1998 .

[11]  Datta Gaitonde,et al.  Multidimensional Collisional Dielectric Barrier Discharge for Flow Separation Control at Atmospheric Pressures , 2005 .

[12]  S. Wilkinson,et al.  Dielectric Barrier Discharge Plasma Actuators for Flow Control , 2010 .

[13]  Matthew G. McHarg,et al.  Plasma-induced force and self-induced drag in the dielectric barrier discharge aerodynamic plasma actuator , 2009 .

[14]  Eric J. Jumper,et al.  Mechanisms and Responses of a Single Dielectric Barrier Plasma Actuator: Plasma Morphology , 2004 .

[15]  Noah Hershkowitz,et al.  Microdischarge propagation and expansion in a surface dielectric barrier discharge , 2008 .

[16]  D. Opaits Dielectric Barrier Discharge Plasma Actuator for Flow Control , 2012 .

[17]  J. Roth,et al.  Electrohydrodynamic Flow Control with a Glow-Discharge Surface Plasma , 2000 .

[18]  James W. Gregory,et al.  Surface Potential and Electric Field Structure in the Aerodynamic Plasma Actuator , 2008 .

[19]  T. Corke,et al.  Separation Control Using Plasma Actuators: Dynamic Stall Vortex Control on Oscillating Airfoil , 2006 .

[20]  C. L. Enloe,et al.  Simulation of the Effects of Force and Heat Produced by a Plasma Actuator on Neutral Flow Evolution , 2006 .

[21]  Guillermo Artana,et al.  Contribution of Plasma Control Technology for Aerodynamic Applications , 2006 .