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攻角影响下的椭锥中心线边界层转捩实验研究

EXPERIMENTAL STUDY ON BOUNDARY LAYER TRANSITION OF ELLIPTICAL CONE CENTERLINE UNDER THE EFFECT OF ANGLE OF ATTACK

  • 摘要: 攻角变化是真实飞行条件下常见的飞行变量之一, 由此引起的流动结构、热力分布等特征变化不可忽视. 为研究攻角对于流向涡失稳相关的三维边界层转捩的影响, 选用长短轴比为4:1的椭锥模型, 针对其迎风面中心线边界层转捩机制及其随攻角变化规律开展了风洞试验研究. 采用温敏漆(TSP)技术与基于纳米示踪的平面激光散射(NPLS)技术, 得到了不同攻角时沿流向方向温升曲线以及流向、横切向的边界层精细结构图像, 分析了转捩起始点、扰动波特征频率以及边界层精细结构随攻角的变化规律, 并基于由脉动压力测试得到的边界层扰动波特征频率和幅值信息对所得规律做了进一步论证与解释. 主要结论如下: 在0 ~ 2°攻角变化范围内, 椭锥中心线边界层均经历了由层流至湍流的演化过程, 边界层转捩过程由低频特征频率主导, 随攻角增大扰动特征频率增大但幅值不变, 且转捩起始点对于攻角的变化不敏感, 而当攻角增大至5°时, 在观测范围内边界层能维持扰动波的稳定增长, 边界层未演变至湍流阶段, 转捩明显推迟.

     

    Abstract: The change in angle of attack is one of the common flight variables under real flight conditions, and the resulting changes in flow structure, the distribution of heat and force, and other characteristics cannot be ignored. To investigate the effect of angle of attack on the three-dimensional boundary layer transition related to streamwise vortex instability, an elliptical cone model with a long to short axis ratio of 4:1 is selected. Wind tunnel experiments are conducted to study the mechanism of boundary layer transition on the windward centerline and its variation with angle of attack. Using Temperature Sensitive Paint (TSP) technology and Nano-tracer based Planar Laser Scattering (NPLS) technology, temperature rise curves along the streamwise direction and fine structure images of the boundary layer in the streamwise and transverse directions are obtained at different angles of attack. The transition starting point, disturbance wave characteristic frequency, and the variation law of fine boundary layer structure with angle of attack are analyzed. Based on the characteristic frequency and amplitude information of boundary layer disturbance waves obtained from pulsating pressure testing, the obtained laws are further demonstrated and explained. The main conclusions are as follows: when the angle of attack varies from 0° to 2° , the boundary layer of the elliptical cone centerline undergoes an evolution from laminar to turbulence. The transition process of the boundary layer is dominated by low-frequency characteristic frequencies, and the disturbance characteristic frequency increases with the increase of angle of attack but the amplitude remains unchanged. The starting point of transition is not sensitive to the changes in angle of attack. However, when the angle of attack increases to 5°, the boundary layer can maintain stable growth of disturbance waves within the observation range, and the transition is significantly delayed without the boundary layer evolving to the turbulence stage.

     

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