航空学报 > 1982, Vol. 3 Issue (1): 45-49

压气机叶栅中的激波附面层相互作用

余申   

  1. 中国科学院工程热物理研究所
  • 收稿日期:1981-06-01 修回日期:1900-01-01 出版日期:1982-03-25 发布日期:1982-03-25

SHOCK WAVE BOUNDARY LAYER INTERACTION IN COMPRESSOR CASCADES

Yu Shen   

  1. Institute of Engineering Thermo physics, Chinese Academy of Sciences
  • Received:1981-06-01 Revised:1900-01-01 Online:1982-03-25 Published:1982-03-25

摘要: 压气机叶栅中激波附面层相互作用是十分复杂的问题,由于相互作用引起分离是决定跨音速压气机性能的重要因素之一。然而迄今为止,尚未深入进行过压气机叶栅激波附面层相互作用的研究,发表的文献极少。作者经过计算和分析,说明压气机叶栅流中主要的相互作用形式是叶栅槽道中激波和湍流附面层的相互作用。作者通过分析指出,研究压气机叶栅激波附面层相互作用,不能直接应用Pearcey分离准则。作者并提出了适用于压气机叶栅的分离准则的函数关系为f(M_1,p_1/p_(L.E.),P_(r.E.)/p_2,Re_0)=O。

Abstract: Shock wave boundary layer interaction in compressor cascades is an extremely complicated problem. In case of the existance of the separation, it is one of the most important factors which determine the performances of transonic compressor.However, no thorough investigation has been made on shock wave boundary layer interaction in compressor cascades and only a few papers on this topic have been published.It is shown by calculation and analysis that the main form of the interaction in compressor cascades is the interaction between shock wave and turbulent boundary layer in channels.The analysis has made clear that the separation criterion proposed by Pearcey is an empirical criterion obtained from wind tunnel tests of a RAE102 airfoil. The conditions are quite different from the restrained channel flow in compressor cascades with strong adverse pressure gradient. As for compressor cascades, the boundary layer grows rapidly and separates at lower Mach number upstream of the shock wave, the length of separated region and the location of vortex sheet are all different from those in the case of Pearcey's single airfoil. The conclusion has been drawn that it is inappropriate to apply Pearcey's separation criterion directly to shock wave boundary layer interaction in compressor cascades.It is proposed that the separation criterion for shock wave boundary layer interaction in compressor cascades be in the form f (M1, p1/p1.E., pT.E./p2,Rec) = 0 , which involves the effects of pressure gradients in front of and behind the shock wave.