MODIFICATIONS OF THE SHEAR LAYER DOWNSTREAM A BACKWARD FACING STEP BY DIELECTRIC BARRIER DISCHARGE PLASMA ACTUATOR

P. Sujar-Garrido, N. Benard, E. Moreau, J. Bonnet
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引用次数: 2

Abstract

The present article deals with a free shear layer induced by the separation of a turbulent boundary layer due to wall divergence. The investigated flow configuration is produced by a 30-mm-height backwardfacing-step mounted in a closed-loop wind tunnel. The experimental measurements are performed at 15 m/s , corresponding to a Reynolds number (based on this velocity and the step height) around 3x10. The modifications of the shear layer are achieved with a surface plasma actuator based on a single Dielectric Barrier Discharge (DBD). This actuator produces an electrohydrodynamic force, resulting in a flow called electric wind just upstream the flow separation. The plasma discharge is able to manipulate the first stages of the formation of the free shear layer and consequently to modify the flow dynamics, highlighting the control authority of plasma discharge. Time-averaged and time-resolved measurements techniques are used to investigate the influence of plasma device in two ways. The first one considers the modification of mean reattachment length whereas the second one studies the effect over large-scale structures. INTRODUCTION Free and bounded turbulent shear flows are intensively studied. The turbulent energy balance splits these flows in two generic configurations: wall-bounded and free shear layers. These two types of flow are usually found in the nature and also in a variety of engineering applications. Knowledge of the flow and the ability to control it are fundamental topics in turbulence. This paper is devoted to the characterization of a free shear layer produced by turbulent boundary layer separation and manipulated by a plasma actuator. The massively separated flow is yield by a sudden wall expansion. The sharp step corner is the fixed location where separation occurs and the location where KelvinHelmholtz instability mechanism begins. The whole process is dominated by the structures arising from this instability (Ho & Huerre, 1984). The effects presented here influence not only the mean flow but also these organized large-scale flow structures. In some extend, the particular ‘step’ flow can be compared with the canonical plane mixing layer case. Their characteristics are very similar in the initial region of the free shear layer but further downstream, the growth and evolution of the free shear layer are affected by the presence of the wall downstream in the case of the BFS. A recirculating region forms and feeds continuously the shear layer producing an increase on the overall turbulence (Adams & Johnston, 1988). Another important feature of a backward facing step flow is the unsteady and highly three-dimensional location of the reattachment point. The dynamic of the separated flow is directly linked with this unsteadiness (Driver et al., 1987). The objective of this study is to investigate the ability of plasma actuators as an effective device for modifying (manipulating) the shear layer, with the final objective of being able to control/reduce the parasitic effects such as unsteadiness, noise, etc. A surface non-thermal plasma discharge is used as flow control device which is now recognized for being effective in different aerodynamic configurations (Benard & Moreau, 2012). This device adds a volume force resulting in a secondary flow, usually called electric wind. Its amplitude and frequency are directly linked to the electrical input signal, this being of primary interest for studying the influence of localized periodic or non-periodic flow perturbations. After the details of the experimental configuration used and the inlet parameters, two main analyses are presented: a parametric study to determine the most effective actuation and a dynamic study of the natural step flow organization. The last part corresponds to a detailed analysis of the particular effective actuation.
用介质阻挡放电等离子体作动器修饰后向台阶下游的剪切层
本文讨论了湍流边界层因壁面散度而分离所引起的自由剪切层。所研究的流动形态是由安装在闭环风洞中的30 mm高的后向台阶产生的。实验测量以15米/秒的速度进行,对应于约3x10的雷诺数(基于此速度和台阶高度)。剪切层的修改是通过基于单介质阻挡放电(DBD)的表面等离子体驱动器实现的。这种执行器产生一种电流体动力,产生一种叫做电风的气流,正好在气流分离的上游。等离子体放电能够控制自由剪切层形成的第一阶段,从而改变流动动力学,突出了等离子体放电的控制权威。采用时间平均和时间分辨测量技术,从两个方面研究了等离子体器件的影响。前者考虑的是平均再附着长度的修正,而后者研究的是在大尺度结构上的影响。对自由和有界湍流剪切流进行了深入研究。湍流能量平衡将这些流动分成两种一般形态:有壁层和自由剪切层。这两种类型的流动通常存在于自然界和各种工程应用中。紊流的知识和控制能力是紊流的基本主题。本文研究了由湍流边界层分离产生的等离子体驱动的自由剪切层的特性。大量分离流是由壁面突然膨胀产生的。陡坡角是分离发生的固定位置,也是KelvinHelmholtz不稳定机制开始的位置。整个过程是由这种不稳定性产生的结构所主导的(Ho & Huerre, 1984)。这些效应不仅影响平均流场,也影响这些有组织的大尺度流场结构。在某种程度上,这种特殊的“阶梯”流可以与典型的平面混合层流进行比较。它们的特征在自由剪切层的初始区域非常相似,但在进一步下游,自由剪切层的生长和演变受到下游壁面存在的影响。一个再循环区域形成并不断供给剪切层,使整体湍流度增加(Adams & Johnston, 1988)。后面向阶跃流动的另一个重要特征是再附着点的非定常和高度三维的位置。分离流的动态与这种不稳定性直接相关(Driver et al., 1987)。本研究的目的是研究等离子体致动器作为修改(操纵)剪切层的有效装置的能力,最终目标是能够控制/减少寄生效应,如不稳定、噪声等。表面非热等离子体放电被用作流动控制装置,现在被认为在不同的气动配置下是有效的(Benard & Moreau, 2012)。这个装置增加了一个体积力,导致二次流,通常称为电风。它的振幅和频率直接与电输入信号有关,这是研究局部周期或非周期流动扰动影响的主要兴趣。在详细介绍了所使用的实验结构和入口参数之后,提出了两项主要分析:确定最有效驱动的参数研究和自然阶跃流动组织的动态研究。最后一部分对应于具体有效作动机构的详细分析。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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