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Experimental and numerical investigation on the surface charge distribution in a Dielectric Barrier Discharge fluid- dynamics plasma actuator.

机译:介质阻挡放电流体动力学等离子体致动器中表面电荷分布的实验和数值研究。

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The Electro-Hydro-Dynamics (EHD) interaction, induced by a dielectric barrier discharge (DBD) in the aerodynamic boundary layer induced in a one atmosphere still air, has been studied both numerically and experimentally. Three different geometrical actuator configurations have been used. The first one is constituted by an electrode pair separated by a 2 mm dielectric teflon sheet. The second and the third configuration have been obtained by adding a third electrode on the upper dielectric surface. This electrode has been placed downstream of the upper electrode and has been connected to the ground or has been left floating. The high voltage electrode has been fed by an a.c. electrical signal. Measurements of the dielectric surface potential generated by the charge deposition have been obtained by using an electrostatic voltmeter. Numerical simulations allowed to determine the charge distribution on the dielectric surface. The discharge has been switched off after positive and negative values of the plasma current. The measurements have been carried out after both phases. Surface potential distributions show that the charge build up takes place several centimeters downstream the upper electrode after the end of the plasma extension. The charge distribution strongly depends on the switching off phase and is heavily affected by the geometrical configuration. Velocity profiles are obtained by using a Pitot probe. They show that the third electrode limits the fluid dynamics performance of the actuator. A relation between the charge surface distribution and the EHD interaction phenomenon has been found. Images of the plasma have been taken to evaluate the discharge structure and the extension of the plasma in the different geometrical configurations studied.
机译:已经通过数值和实验研究了由在一种大气静止的空气中引起的空气动力学边界层中的介电势垒放电(DBD)引起的电水动力(EHD)相互作用。已经使用了三种不同的几何致动器配置。第一个电极由一对电极隔开,电极对被2毫米的聚四氟乙烯薄片隔开。通过在上介电表面上添加第三电极来获得第二和第三构造。该电极已放置在上部电极的下游,并已接地或悬空。高压电极由交流电供电。电信号。通过使用静电伏特计已经获得了由电荷沉积产生的介电表面电势的测量值。数值模拟可以确定介电表面上的电荷分布。在等离子电流为正值和负值之后,放电已关闭。在两个阶段之后都进行了测量。表面电势分布表明,在等离子扩展结束后,电荷积累发生在上部电极的下游几厘米处。电荷分布在很大程度上取决于关断相位,并且受几何形状的影响很大。速度轮廓是通过使用皮托管探针获得的。他们表明,第三电极限制了执行器的流体动力学性能。已经发现电荷表面分布与EHD相互作用现象之间的关系。已经拍摄了等离子体的图像以评估所研究的不同几何构型下的放电结构和等离子体的延伸。

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