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Shear-flow excitation mechanisms of recessed localized arc-filament plasma actuators

机译:凹入式局部电弧丝等离子体致动器的剪切流激励机制

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Localized arc-filament plasma actuators, placed near the nozzle lip of a laboratory jet, have recently been demonstrated to have sufficient control authority to significantly excite the jet downstream [M. Samimy et al., J. Fluid Mech.578, 305 (2007)]. This class of plasma actuator, which in this application is recessed in a small cavity near the nozzle lip, causes intense local heating. This heating is thought to be the root mechanism of its influence on the flow, but how this principally entropic thermal source couples with the vortical jet shear layer turbulence downstream is unclear. We investigate this using direct numerical simulations, which match the flow conditions of the corresponding experiment, including Reynolds number, but are two-dimensional to ease computational expense. Despite this obvious modeling approximation, the simulations include the key features of the laboratory system: a thin boundary layer, a plasma-like thermal source in a small recessed cavity, a nozzle lip, and a downstream free shear layer. Results are shown to match the temperature and near-field pressure measured in the laboratory actuators. It is found that the cavity, which was initially included to shield the actuator plasma from the flow, is essential for its action. Thermal expansion within the cavity leads to an ejection of fluid from it, which perturbs the boundary layer and the downstream mixing layer. There is a finite baroclinic torque, but its effects are relatively minor. An alternate actuator designed to mimic the pressure effects of the full actuator, without its concomitant thermal heating, is nearly as effective at exciting the shear layer. An actuator model without the cavity recess does not provide effective actuation. These results suggest that there is significant potential to optimize the actuation authority through design of cavity recesses that augment its effect.
机译:最近已证明,放置在实验室喷嘴的喷嘴唇附近的局部电弧丝等离子体致动器具有足够的控制权,可以显着地激发下游的喷嘴[M。 Samimy等人,J.Fluid Mech.578,305(2007)。此类等离子致动器(在此应用中凹入喷嘴唇附近的小腔中)会引起强烈的局部加热。人们认为这种加热是其影响流动的根本原因,但目前尚不清楚这种主要的熵热源如何与下游的涡流射流剪切层湍流耦合。我们使用直接数值模拟来研究此问题,该数值模拟与相应实验的流动条件(包括雷诺数)相匹配,但为二维计算以减轻计算费用。尽管有这种明显的建模近似,但模拟仍包含实验室系统的关键特征:薄边界层,小凹腔内的等离子体热源,喷嘴唇和下游自由剪切层。显示的结果与实验室执行器中测得的温度和近场压力相匹配。已经发现,最初用于保护执行机构等离子体不受流动影响的腔对于其作用至关重要。空腔内的热膨胀导致流体从空腔中喷出,从而扰乱了边界层和下游混合层。斜压转矩是有限的,但是其影响相对较小。设计为模仿整个执行器的压力效应而无需伴随加热的替代执行器,在激发剪切层方面几乎同样有效。没有空腔凹槽的执行器模型无法提供有效的执行器。这些结果表明,通过设计腔凹部以增强其作用,有优化驱动机构的巨大潜力。

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