由喷射进主流的扫射射流形成的流动结构

M. Fuchiwaki, S. Raghu
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引用次数: 1

摘要

人们提出了各种控制流动分离的方法,并对与流动状态相对应的主动分离控制进行了许多研究。然而,它们的效率一直受到电力需求的阻碍。最近报道了一种不需要电力的基于流体振荡器的主动流动分离控制装置。该装置能够在宽空间范围内产生扫射射流以及流体振荡,其内部结构消除了对驱动单元的需求。本文报道了利用流体振荡器进行流动分离控制技术的研究。然而,这些结果大多是从流动控制的角度对动力的贡献,对利用流体振荡器控制分离流动的流动机理的研究尚不清楚。特别是射流振荡器的扫射射流与主流的相互作用以及由此产生的流动结构,目前还不清楚。为了利用射流振荡器制造高效的流动分离控制装置,需要通过射流振荡器的扫射射流与主流的相互作用来理解复杂的流动结构。本研究的目的是利用立体PIV测量方法定量研究射流振荡器的扫射射流与主流相互作用下的流动结构。射流振荡器喷出的扫射射流在高速比下明显破坏了主流,导致流动结构发生了显著变化。高速射流出现在结构的中心部分,伴随着低速流在外部,形成三维分布。射流振荡器喷出的扫射射流在高速比下保持两流相互作用的扩散角。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Flow Structure Formed by a Sweeping Jet Ejected Into a Main Flow
Various methods of controlling flow separation have been proposed and many studies have been performed on active separation control in correspondence with the flow state. However, their efficiency has been hampered by the requirement of electric power for the added stream. Recently, an active flow separation control device based on a fluidic oscillator that does not require electric power has been reported. This device is able to generate a sweeping jet over a wide spatial range as well as fluid oscillations, and its internal structure eliminates the need for a drive unit. The studies of the flow separation control techniques using the fluidic oscillator have been reported. However, most of these results are mainly contribution of the dynamic forces from the viewpoint of the flow control and the study on the flow mechanism for the separation flow control using the fluidic oscillator have not been understood. Especially, it is not known the interaction between the sweeping jet from the fluidic oscillator and the main flow and the flow structure due to the interaction. In order to make a flow separation control devise with high efficiency using the fluidic oscillator, it is require to be understood the complex flow structure by the interaction between the sweeping jet from the fluidic oscillator and the main flow. The purpose of the present study is to investigate the flow structure by the interaction between the sweeping jet from the fluidic oscillator and the main flow quantitatively by the stereo PIV measurement. The sweeping jet ejected from a fluidic oscillator evidently disrupts the main flow at high velocity ratios, leading to a significant change in flow structure. A high-speed jet appears at the center part of the structure, accompanied by low-speed flow at the outside, producing a 3D distribution. The sweeping jet ejected from the fluidic oscillator maintains the spreading angleas a result of the interaction between the two flows at high velocity ratios.
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