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Micro vortex generator control of axisymmetric high-speed laminar boundary layer separation

机译:轴对称高速层流边界层分离的微涡发生器控制

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Interest in the development of micro vortex generators (MVGs) to control high-speed flow separation has grown in the last decade. In contrast to conventional vortex generators, MVGs are fully submerged in the boundary layer and have the potential of inducing surface flow mixing with marginal drag penalty when suitably designed. Also, they do not result in undesired reduced mass flow such as with suction methods. The flow mechanisms at the location of MVGs are not yet fully understood, and optimal designs are difficult to establish given that both numerical predictions and experiments are particularly challenged for short element heights, yet optimal MVGs are generally expected to be at least shorter than half the local boundary layer thickness. The present work aims at investigating experimentally the fundamental flow physics concerning an individual MVG element (of 'canonical' or simplified geometry) at a range of near-wall heights. A fully laminar base flow is considered so as to isolate the effect of incoming turbulence as well as the more complex physics that may occur when specific and/or multiple elements are used. Tests were performed in a gun tunnel at a freestream Mach number of 8.9 and Reynolds number of /m, and the basic test model consisted of a blunt-nosed cylinder which produced an axisymmetric laminar boundary layer with an edge Mach number of 3.4 and Reynolds number of /m at the MVG location. A laminar shock-wave/boundary layer interaction with separation was induced by a flare located further downstream on the model. Measurements consisted of time-resolved surface heat transfer obtained in the axial direction immediately downstream of the MVG and along the interaction, together with simultaneous high-speed schlieren imaging. The height () of the MVG element used in a 'diamond' configuration (square planform with one vertex facing the flow) was adjusted between tests ranging from = 0.03 to 0.58, where the local undisturbed boundary layer thickness was = 1.75 mm. The effect of planform geometry was further assessed by performing tests with the MVG used in a 'square' configuration (one edge normal to the incoming flow). Results show that MVG height drives the intensification of heat transfer fluctuations in the wake of the element. The optimal MVG operating conditions, where downstream boundary layer separation is avoided and minimal flow interference is produced, based here on heat transfer unsteadiness, are with a 'diamond' arrangement.
机译:在过去的十年中,人们对开发微涡旋发生器(MVG)以控制高速流分离的兴趣不断增长。与传统的涡流发生器相比,MVGs完全浸没在边界层中,并且在进行适当设计时具有潜在的引起表面流混合以及边际阻力损失的潜力。而且,它们不会导致不希望的质量流减少,例如采用抽吸方法。尚未完全了解MVG位置的流动机理,并且鉴于数值预测和实验都对短元素高度特别有挑战,因此很难建立最佳设计,但是通常期望最佳MVG至少短于一半的高度。局部边界层厚度。本工作旨在通过实验研究有关单个MVG元素(“规范”或简化几何形状)在近壁高度范围内的基本流动物理学。考虑使用完全层流基流,以便隔离传入湍流的影响以及使用特定和/或多个元素时可能发生的更复杂的物理现象。测试在自由通道马赫数为8.9,雷诺数为/ m的喷枪隧道中进行,基本测试模型由钝头圆柱体组成,该圆柱头产生了轴对称层状边界层,边缘马赫数为3.4和雷诺数/ m在MVG位置。层流激波/边界层与分离的相互作用是由位于模型下游的火炬引起的。测量包括在MVG的紧下游沿轴向并沿着相互作用获得的时间分辨的表面传热,以及同时进行的高速schlieren成像。在“钻石”配置(方形平面,一个顶点面向流动)中使用的MVG元件的高度()在介于0.03到0.58之间的测试之间进行了调整,其中局部未扰动的边界层厚度为1.75 mm。通过以“正方形”配置(垂直于输入流的一条边)使用MVG进行测试,可以进一步评估平面几何形状的影响。结果表明,MVG高度驱动元件尾流传热波动的加剧。最佳的MVG操作条件是“菱形”布置,可避免下游边界层分离,并根据传热的不稳定性产生最小的流动干扰。

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