HyTRV标模下表面高速边界层转捩实验研究

Experimental investigation of high-speed boundary layer transition mechanisms on the HyTRV model

  • 摘要: HyTRV标模边界层转捩具有复杂的三维性。为深入认识HyTRV标模下表面横流区和中心线区域边界层转捩机理,在马赫6低噪声实验平台(SKLA-TT1)开展了实验研究。采用红外热成像技术获得了−2°、0°、2°和4°攻角下边界层转捩阵面,进一步采用高频压力脉动传感器研究了0°和2°攻角下边界层扰动波演化过程,并采用瑞利散射流动显示技术和粒子图像测速(PIV)技术进行了流动可视化与速度场测量。红外测量结果显示,下表面转捩阵面呈“双肺叶”状分布,转捩区域可分为横流区和中心线区域。在0°攻角时,横流区存在200~500 kHz的宽频扰动,结合瑞利散射流动显示结果,判断其为高频的横流二次失稳模态。中心线区域未测到明显的扰动信号,但PIV测量结果显示边界层内存在剪切层和涡结构。攻角增大至2°时,高频二次失稳模态的幅值降低且频带向低频方向偏移,中心线区域转捩位置前移。实验结果表明,模型下表面横流区边界层转捩由高频的非定常横流波二次失稳模态主导,攻角增大会削弱横流效应,导致转捩阵面后移;中心线区域转捩由流向涡失稳主导,攻角增大会导致转捩位置前移。

     

    Abstract: The boundary layer transition (BLT) of the HyTRV (Hypersonic Transition Research Vehicle) model exhibits complex three-dimensional characteristics. Experiments have been conducted in the Mach 6 low-noise wind tunnel named SKLA-TT1 to investigate BLT on the bottom surface of HyTRV model, specifically within the crossflow region and centerline region. Infrared thermography was used to obtain the transition front distribution at angles of attack of −2°, 0°, 2°, and 4°. High-frequency pressure sensors were employed to study the evolution of disturbance waves at 0° and 2° angles of attack. In addition, flow visualization and velocity field measurements were conducted using Rayleigh scattering and particle image velocimetry (PIV). It was found that a distinct ‘double-lobed’ transition front on the bottom surface was visualized by Infrared thermography. The transition region was divided into the crossflow region and the centerline region. At 0° case, high-frequency disturbances ranging from 200 to 500 kHz in the crossflow region were detected by high-frequency pressure sensors and visualized by Rayleigh scattering technique, which were determined to be the secondary instability modes of unsteady crossflow. No obvious dominant frequency was observed in the centerline region, whereas shear layers and vortex structures were obtained by PIV technique within the boundary layer. At 2° case, the amplitude of high-frequency secondary instability decreased with a frequency shifting towards lower bands compared to the 0° case, and the transition location in centerline region shifts upstream. Thus, it is found that BLT in the crossflow region is dominated by high-frequency secondary instability of unsteady crossflow. Increasing the angle of attack weakens the crossflow instability and makes the transition front move downstream. Conversely, transition along the centerline region is governed by streamwise vortex instability. Besides the transition onset moves upstream at higher angles of attack.

     

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