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ON THE FLOW AND TURBULENCE WITHIN THE WAKE AND BOUNDARY LAYER OF A ROTOR BLADE LOCATED DOWNSTREAM OF AN IGV

机译:IGV转子叶片下部流尾流和边界层内的流动和湍流

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This paper presents detailed experimental data on the flow and turbulence within the wake and boundary layer of a rotor blade operating behind a row of Inlet Guide Vanes (IGVs). The experiments are performed in a refractive index matched facility that provides an unobstructed view of the entire flow field. Results of the high-resolution 2D Particle Image Velocimetry (PIV) measurements are used for characterizing the mean flow, Reynolds stresses, turbulent kinetic energy as well as dissipation and production rates. Dissipation and production rates are high and of the same order of magnitude near the trailing edge, and decrease rapidly with increasing distance from the blade. The trend is reversed in the wake kinking region, resulting in elevated turbulence levels, i.e. a turbulent hot spot. One-dimensional spectral analysis shows that, except for the very near wake and hot-spot regions, the turbulence within the rotor wake can be assumed to be isotropic. Also the directions of the maximum shear strain and shear stress are aligned in that region, i.e. consistent with eddy viscosity type Reynolds stress models. The rotor near wake mainly consists of two parallel layers experiencing planar shear with opposite signs as one would expect to find in a 2D wake. However, orientation differences can extend up to 45° near the trailing edge and the hot-spot. Furthermore, there is substantial mismatch in the location of the local maxima of stresses and strains. The values of S_(33) are also large there, indicating that the flow is three-dimensional. Rotor boundary layer measurements focus on a region where the IGV wake intersects with the rotor blade. The impingement of the increased axial velocity region in between the IGV wakes causes the thinning of the boundary layer. This is similar to the effect of a turbulent jet impinging on a flat surface. When viewed in the frame of reference of "non-wake" flow regions, the boundary layer thinning can also be attributed to the suction (or "negative jet") effect of the "slip velocity" present in the IGV wake segments. Spectral analysis shows that the turbulence in the rotor boundary layer is highly anisotropic. As a result, the spectra cannot be used for estimating the dissipation rate.
机译:本文介绍了在一排进口导流叶片(IGV)后面运行的转子叶片的尾流和边界层内的流动和湍流的详细实验数据。实验是在折射率匹配的设备中进行的,该设备提供了整个流场的一览无遗的视图。高分辨率2D粒子图像测速(PIV)测量的结果用于表征平均流量,雷诺应力,湍动能以及耗散率和生产率。耗散率和生产率很高,并且在后缘附近处于相同数量级,并且随着距叶片距离的增加而迅速降低。在尾流弯折区域这种趋势被逆转,导致湍流水平升高,即湍流热点。一维频谱分析表明,除了非常接近的尾流和热点区域外,可以将转子尾流内的湍流假定为各向同性。在该区域内,最大剪切应变和剪切应力的方向也对齐,即与涡流粘度型雷诺应力模型一致。接近尾流的转子主要由两个平行的层组成,它们经受平面剪切并具有相反的符号,正如人们希望在二维尾波中发现的那样。但是,方向差异可以在后缘和热点附近延伸至45°。此外,在应力和应变的局部最大值的位置上存在很大的不匹配。 S_(33)的值在那里也很大,表明流是三维的。转子边界层测量的重点是IGV尾流与转子叶片相交的区域。 IGV尾流之间增加的轴向速度区域的撞击导致边界层变薄。这类似于湍流射流撞击在平坦表面上的效果。当在“非苏醒”流动区域的参照系中观察时,边界层变薄也可归因于IGV苏醒段中存在的“滑移速度”的吸力(或“负射流”)效应。光谱分析表明,转子边界层中的湍流是高度各向异性的。结果,光谱不能用于估计耗散率。

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