4.6 Article

Influence of shock waves from plasma actuators on transonic and supersonic airflow

Journal

JOURNAL OF PHYSICS D-APPLIED PHYSICS
Volume 51, Issue 10, Pages -

Publisher

IOP PUBLISHING LTD
DOI: 10.1088/1361-6463/aaa838

Keywords

plasma actuator; blast waves; CFD simulation; surface discharge; flow visualization

Funding

  1. RFBR [17-08-00560, 17-08-00909]

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This paper presents experimental and numerical investigations of high-current sliding surface discharges of nanosecond duration and their effect on high-speed flow as plasma actuators in a shock tube. This study deals with the effectiveness of a sliding surface discharge at low and medium air pressure. Results cover the electrical characteristics of the discharge and optical visualization of the discharge and high-speed post-discharge flow. A sliding surface discharge is first studied in quiescent air conditions and then in high-speed flow, being initiated in the boundary layer at a transverse flow velocity of 50-950 m s(-1) behind a flat shock wave in air of density 0.04-0.45 kg m(-3). The discharge is powered by a pulse voltage of 25-30 kV and the electric current is similar to 0.5 kA. Shadow imaging and particle image velocimetry (PIV) are used to measure the flow field parameters after the pulse surface discharge. Shadow imaging reveals shock waves originating from the channels of the discharge configurations. PIV is used to measure the velocity field resulting from the discharge in quiescent air and to determine the homogeneity of energy release along the sliding discharge channel. Semicylindrical shock waves from the channels of the sliding discharge have an initial velocity of more than 600 m s(-1). The shock-wave configuration floats in the flow along the streamlined surface. Numerical simulation based on the equations of hydrodynamics matched with the experiment showed that 25%-50% of the discharge energy is instantly transformed into heat energy in a high-speed airflow, leading to the formation of shock waves. This energy is comparable to the flow enthalpy and can result in significant modification of the boundary layer and the entire flow.

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