Computational  Modelling  of  Unsteady  Airfoil  Flows

Dynamic Airfoil Stall

The most prominent example of dynamic airfoil stall refers to helicopters under forward or maneuvering flight conditions. Here, the incidence of the rotor blade sections periodically changes from moderate up to fairly large values. In contrast to steady-state airfoil stall, the rapidly increasing incidence usually delays the onset of stall to regimes which may exceed the static stall angle by a significant amount. However, once dynamic stall occurs, the aerodynamic loads are generally more severe compared to steady stall and may cause significant increases in the blade stresses and the control system loads. Due to the complexity of the involved flow-physics (e.g. reverse transition) an accurate numerical prediction of dynamic stall in the frame of RANS is quite challenging.

Figure 3: Lift- and Pitching moment coefficient in the case of dynamic stall (Ekaterinaris [3])


Numerous experiments have revealed the sequence of flow events depicted in Figure 1 taken from Ekaterinaris [3]. First, a vortex starts to develop near the airfoil leading edge as the angle of attack is rapidly increased past the static stall angle. This vortex then is convected downstream near the airfoil surface which causes an increase in lift due to the suction induced by the vortex. The magnitude of the lift increase depends on the strength of the vortex and its distance from the surface. The streamwise movement of the vortex depends on the airfoil shape and the pitch rate. As the vortex is convected past the trailing edge, the pitching moment briefly attains its maximum negative value and then both lift and pitching moment start to drop rapidly. The flow over the airfoil remains stalled until the angle of attack has decreased sufficiently to enable flow reattachment. As a result of this sequence of flow events, the unsteady lift, drag, and pitching moment coefficients show a large degree of flow hysteresis when plotted as a function of incidence angle. The amount of hysteresis and the shape of the hysteresis loops vary in a highly non-linear fashion with the amplitude of oscillation, mean angle of attack and reduced frequency of oscillation.



Background Dynamic Stall Comp. Approach Results Animations

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Last modified: Thu Feb 10 10:26:53 CET 2000