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Rotor boundary layer development with inlet guide vane (IGV) wake impingement

机译:转子边界层开发与入口导向叶片(IGV)唤醒撞击

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This paper examines the transition process in a boundary layer on a rotor blade under the impingement of an inlet guide vane wake. The effects of wake strengths and the reduced frequency on the unsteady boundary layer development on a low-speed axial compressor were investigated using particle image velocimetry. The measurements were carried out at two reduced frequencies (f(r) = integral (IGV) S-0/U-2i, f(r) = 1.35, and f(r) = 0.675) with the Reynolds number, based on the blade chord and the isentropic inlet velocity, being 97 500. At f(r) = 1.35, the flow separated at the trailing edge when the wake strength was weak. However, the separation was almost totally suppressed as the wake strength increased. For the stronger wake, both the wake's high turbulence and the negative jet behavior of the wake dominated the interaction between the unsteady wake and the separated boundary layer on the suction surface of the airfoil. The boundary layer displacement thickened first due to the negative jet effect. Then, as the disturbances developed underneath the wake, the boundary layer thickness reduced gradually. The high disturbance region convected downstream at a fraction of the free-stream velocity and spread in the streamwise direction. The separation on the suction surface was suppressed until the next wake's arrival. Because of the long recovery time at f(r) = 0.675, the boundary layer thickened gradually as the wake convected further downstream and finally separated due to the adverse pressure gradient. The different boundary layer states in turn affected the development of disturbances. Published by AIP Publishing.
机译:本文在入口导向叶片瓶的冲击下检查转子叶片上的边界层中的过渡过程。使用粒子图像测速研究了唤醒强度和频率降低频率对低速轴向压缩机上的不稳定边界层开发的影响。基于的雷诺数叶片和弦和型熵入口速度,为97 500.在f(r)= 1.35处,当唤醒强度较弱时,在后缘处分离在后缘。然而,随着唤醒强度的增加,分离几乎完全抑制。对于唤醒唤醒,唤醒的高湍流和唤醒的负射流行为占主导地位在翼型的吸入表面上的不稳定唤醒和分离边界层之间的相互作用。由于负射流效果,边界层位移首先增厚。然后,随着在唤醒下方发生的干扰,边界层厚度逐渐减小。高扰动区域在自由流速度的一小部分处与下游进行下游,并在流动方向上展开。吸入表面上的分离被抑制直到下一个唤醒到达。由于F(R)= 0.675的长恢复时间,边界层随着在进一步下游的进一步处理的情况下逐渐增厚,并且由于不利的压力梯度而最终分离。不同的边界层状态反过来影响了干扰的发展。通过AIP发布发布。

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