Boundary Layer Control with a Plasma Actuator Utilizing a Large GND Mesh Electrode and Two HV Electrode Configurations

This article presents the results of experimental studies on the influence of the geometry of high-voltage plasma actuator electrodes on the change in flow in the boundary layer and their influence on the change in the lift coefficient. The plasma actuator used in the described experimental studies...

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Main Authors: Ernest Gnapowski, Sebastian Gnapowski, Paweł Tomiło
Format: Article
Language:English
Published: MDPI AG 2024-12-01
Series:Sensors
Subjects:
Online Access:https://www.mdpi.com/1424-8220/25/1/105
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author Ernest Gnapowski
Sebastian Gnapowski
Paweł Tomiło
author_facet Ernest Gnapowski
Sebastian Gnapowski
Paweł Tomiło
author_sort Ernest Gnapowski
collection DOAJ
description This article presents the results of experimental studies on the influence of the geometry of high-voltage plasma actuator electrodes on the change in flow in the boundary layer and their influence on the change in the lift coefficient. The plasma actuator used in the described experimental studies has a completely different structure. The experimental model of the plasma actuator uses a large mesh ground electrode and different geometries of the high-voltage electrodes, namely copper solid electrodes and mesh electrodes (the use of mesh electrodes, large GND and HV is a new solution). The plasma actuator was placed directly on the surface of the wing model with the SD 7003 profile. The wing model with the plasma actuator was placed in the wind tunnel. All experimental tests carried out were carried out for various configurations. The DBD plasma actuator was powered by a high-voltage power supply with a voltage range from <i>V<sub>p</sub></i> = 7.5–15 kV. The use of a high-voltage mesh electrode allowed for an increase in the lift coefficient (C<sub>L</sub>) for the angle of attack <i>α</i> = 5 degrees and the air flow velocity in the range from <i>V</i> = 5 m/s to 20 m/s, while the use of copper electrodes HV with the plasma actuator turned off and on, were very small (close to zero). The experimental studies were conducted for Reynolds numbers in the range of Re = 87,985–351,939.
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issn 1424-8220
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spelling doaj-art-64d67aacb81d477186b3831fdb9100792025-08-20T02:47:13ZengMDPI AGSensors1424-82202024-12-0125110510.3390/s25010105Boundary Layer Control with a Plasma Actuator Utilizing a Large GND Mesh Electrode and Two HV Electrode ConfigurationsErnest Gnapowski0Sebastian Gnapowski1Paweł Tomiło2Faculty of Mathematics and Information Technology, Lublin University of Technology, 20-618 Lublin, PolandFaculty of Mathematics and Information Technology, Lublin University of Technology, 20-618 Lublin, PolandFaculty of Management, Lublin University of Technology, 20-618 Lublin, PolandThis article presents the results of experimental studies on the influence of the geometry of high-voltage plasma actuator electrodes on the change in flow in the boundary layer and their influence on the change in the lift coefficient. The plasma actuator used in the described experimental studies has a completely different structure. The experimental model of the plasma actuator uses a large mesh ground electrode and different geometries of the high-voltage electrodes, namely copper solid electrodes and mesh electrodes (the use of mesh electrodes, large GND and HV is a new solution). The plasma actuator was placed directly on the surface of the wing model with the SD 7003 profile. The wing model with the plasma actuator was placed in the wind tunnel. All experimental tests carried out were carried out for various configurations. The DBD plasma actuator was powered by a high-voltage power supply with a voltage range from <i>V<sub>p</sub></i> = 7.5–15 kV. The use of a high-voltage mesh electrode allowed for an increase in the lift coefficient (C<sub>L</sub>) for the angle of attack <i>α</i> = 5 degrees and the air flow velocity in the range from <i>V</i> = 5 m/s to 20 m/s, while the use of copper electrodes HV with the plasma actuator turned off and on, were very small (close to zero). The experimental studies were conducted for Reynolds numbers in the range of Re = 87,985–351,939.https://www.mdpi.com/1424-8220/25/1/105plasma actuatorflow controlwing airfoilwind tunnelmesh electrodesDBD
spellingShingle Ernest Gnapowski
Sebastian Gnapowski
Paweł Tomiło
Boundary Layer Control with a Plasma Actuator Utilizing a Large GND Mesh Electrode and Two HV Electrode Configurations
Sensors
plasma actuator
flow control
wing airfoil
wind tunnel
mesh electrodes
DBD
title Boundary Layer Control with a Plasma Actuator Utilizing a Large GND Mesh Electrode and Two HV Electrode Configurations
title_full Boundary Layer Control with a Plasma Actuator Utilizing a Large GND Mesh Electrode and Two HV Electrode Configurations
title_fullStr Boundary Layer Control with a Plasma Actuator Utilizing a Large GND Mesh Electrode and Two HV Electrode Configurations
title_full_unstemmed Boundary Layer Control with a Plasma Actuator Utilizing a Large GND Mesh Electrode and Two HV Electrode Configurations
title_short Boundary Layer Control with a Plasma Actuator Utilizing a Large GND Mesh Electrode and Two HV Electrode Configurations
title_sort boundary layer control with a plasma actuator utilizing a large gnd mesh electrode and two hv electrode configurations
topic plasma actuator
flow control
wing airfoil
wind tunnel
mesh electrodes
DBD
url https://www.mdpi.com/1424-8220/25/1/105
work_keys_str_mv AT ernestgnapowski boundarylayercontrolwithaplasmaactuatorutilizingalargegndmeshelectrodeandtwohvelectrodeconfigurations
AT sebastiangnapowski boundarylayercontrolwithaplasmaactuatorutilizingalargegndmeshelectrodeandtwohvelectrodeconfigurations
AT pawełtomiło boundarylayercontrolwithaplasmaactuatorutilizingalargegndmeshelectrodeandtwohvelectrodeconfigurations