航空学报 > 1990, Vol. 11 Issue (11): 626-629

二维机翼二自由度跨音速颤振分析

姚宇峰   

  1. 上海飞机研究所
  • 收稿日期:1989-10-25 修回日期:1990-04-15 出版日期:1990-11-25 发布日期:1990-11-25

TRANSONIC FLUTTER ANALYSIS OF 2-D AIRFOILS WITH 2 DEGREES OF FREEDOM

Yao Yufeng   

  1. Shanghai Aircraft Design and Research Institute
  • Received:1989-10-25 Revised:1990-04-15 Online:1990-11-25 Published:1990-11-25

摘要: <正> On the assumption that airfoils take small amplitude ha-rmonic oscillating and middle reduced frequency, the two-dimensional, inviscid, small-disturbance nonlinear unsteady transonic flow equation can be split into two parts. One is the nonlinear steady small-disturbance equation, the other is the time-linearized unsteady small-disturbance equation. The steady equation is solved by Carlson code. The unsteady equation is solved by integral method. The standard v-g method is used to solve the flutter eigenvalue equations. A transonic flutter analysis is performed for a NACA 64A006 airfoil with pitching and plunging degrees of freedom.The Mach numbers considered are 0.7, 0.8, and 0.85. The aerodynamic coefficients are obtained by the above method. For each Mach number, the flutter speed and the corresponding flutter reduced frequencies are achieved by varying the airfoil-airmass ratio, plunge-pitch frequency ratio. The results are compared with other computational method and good agreement has been observe

关键词: 翼型, 非定常跨音速流, 跨音速颤振

Abstract: On the assumption that airfoils take small amplitude ha-rmonic oscillating and middle reduced frequency, the two-dimensional, inviscid, small-disturbance nonlinear unsteady transonic flow equation can be split into two parts. One is the nonlinear steady small-disturbance equation, the other is the time-linearized unsteady small-disturbance equation. The steady equation is solved by Carlson code. The unsteady equation is solved by integral method. The standard v-g method is used to solve the flutter eigenvalue equations. A transonic flutter analysis is performed for a NACA 64A006 airfoil with pitching and plunging degrees of freedom.The Mach numbers considered are 0.7, 0.8, and 0.85. The aerodynamic coefficients are obtained by the above method. For each Mach number, the flutter speed and the corresponding flutter reduced frequencies are achieved by varying the airfoil-airmass ratio, plunge-pitch frequency ratio. The results are compared with other computational method and good agreement has been observed.

Key words: airfoil, unsteady transonic flow, transonic flutter