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Effect of Free-Stream Turbulence on the Structure and Dynamics of Laminar Separation Bubbles

机译:自由流湍流对层流分离气泡结构和动力学的影响

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Laminar separation is always associated with considerable unsteadiness. This unsteadiness is caused by large coherent structures that are a consequence of hydrodynamic instability mechanisms of the mean flow. The mean-flow topology and unsteady behavior of laminar separation bubbles (LSB) is in fact mainly governed by instability and transition. In this paper, laminar separation bubbles, which are generated on a flat plate by imposing a streamwise adverse pressure gradient, are investigated by means of Direct Numerical Simulations (DNS). The streamwise pressure gradient for the DNS is chosen such that the inviscid wall pressure distribution, as reported in the Gaster experimental series Ⅰ, case Ⅳ, is closely matched. This case was classified as a "short" laminar separation bubble. The time-averaged flow field obtained from the DNS with no external disturbances introduced (no free-stream turbulence), reveals that the bubble is longer than observed in the experiments. In fact, the bubble obtained in the simulations appeared to be a "long" bubble. This was confirmed by comparing the simulation results with the measurements by Gaster for a long bubble. The discrepancy between the numerical simulations and experiments is possibly due to an earlier onset of transition in the experiments. In the present simulations, instead of forcing with random disturbances to promote transition, isotropic grid turbulence, which was modeled using a superposition of eigenmodes from the continuous spectrum of the Orr-Sommerfeld and Squire operators is introduced at the inflow boundary. It was observed that as the free-stream turbulence (FST) intensity was increased, the bubble became smaller. The separation bubble was in fact shortened from both sides (separation and reattachment sides) in the presence of free-stream turbulence. Comparing the wall pressure distribution for 0.2% free-stream turbulence with Gaster experiment revealed that then the bubble could be classified as a "short" bubble. Based on the simulations performed, FST can change a separation bubbles form "long" to "short". In order to investigate bubble "bursting", the development of bubble, that had became short due to FST, was simulated after the FST was turned-off. The short bubble grew for a short period of time. Surprisingly however, it did not return to the original, state without FST.
机译:层流分离总是伴随着相当大的不稳定。这种不稳定是由大的连贯结构引起的,这是平均流的流体动力不稳定性机制的结果。实际上,层流分离气泡(LSB)的平均流拓扑和非稳态行为主要受不稳定和过渡的支配。在本文中,通过直接数值模拟(DNS)研究了通过施加逆流逆向压力梯度而在平板上产生的层流分离气泡。选择DNS的沿流方向的压力梯度,以使Gaster实验系列Ⅰ(案例Ⅳ)中报告的不粘壁压力分布紧密匹配。该病例被分类为“短”层流分离泡。从DNS获得的时间平均流场,没有引入外部干扰(没有自由流湍流),表明气泡比实验中观察到的更长。实际上,在模拟中获得的气泡似乎是“长”气泡。通过将模拟结果与Gaster的测量结果进行比较(长气泡),可以证实这一点。数值模拟和实验之间的差异可能是由于实验中过渡的开始较早。在当前的模拟中,不是用随机干扰强迫转换,而是在流入边界处引入了各向同性的网格湍流,该湍流是使用来自Orr-Sommerfeld和Squire算子的连续谱的本征模叠加建立的。观察到,随着自由流湍流(FST)强度的增加,气泡变得更小。实际上,在存在自由流湍流的情况下,分离气泡从两侧(分离和重新连接侧)都缩短了。将0.2%自由流湍流的壁面压力分布与Gaster实验进行比较后发现,该气泡可被归类为“短”气泡。基于执行的模拟,FST可以将分离气泡从“长”更改为“短”。为了研究气泡“破裂”,在FST关闭后模拟了由于FST而变短的气泡的产生。短气泡在短时间内增长。但是令人惊讶的是,没有FST,它没有返回到原始状态。

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