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Abstracts - KTH Mechanics

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Dynamic Lift of Airfoils<br />

R. Grüneberger, T. Bohlen, S. Barth and J. Peinke ∗<br />

For airfoils it is known that the lift coefficient cL depends not only on the angle of<br />

attack α but also on the steadiness of the flow. Varying the angle of attack with an<br />

angular velocity ω = ∂α/∂t the lift force for angles larger than the steady stall angle<br />

clearly depends on ω, too,i.e.cL = f(α, ω). Variations of α and ω can be either due<br />

to different pitch angles of the airfoil or due to fluctuations of amplitude and direction<br />

of the flow as it is the case for wind turbines in atmospheric boundary layers.<br />

We present wind tunnel measurements. In order to quantify the dynamic stall<br />

effect, the lift of an FX79-W-151A airfoil, which is for use on wind turbines, is determined<br />

by the integral pressure distribution at the wind tunnel walls while rotating<br />

the airfoil with defined angular velocities ω. The rotation speed is varied by numeric<br />

control. The pressure measurement is performed by two sets of 40 pressure sensors<br />

at each side wall of the wind tunnel. The temporal resolution of the pressure measurement<br />

is in the range of milliseconds. For stochastic analysis the experiment is<br />

repeated several hundred times. In contrast to static lift values, there is an increase<br />

(overshoot) of lift before flow separation on the suction side occurs, dependent on ω,<br />

see Fig 1.<br />

This knowledge of the maximum lift forces is relevant for the estimation of extreme<br />

mechanical loads on wind turbine blades and therefore of special interest for wind<br />

turbine manufacturers.<br />

∗ ForWind - Center for Wind Energy Research - University of Oldenburg<br />

Figure 1: Increase of the maximum lift coefficient cL with increase of the angular<br />

velocity ω =˙α.<br />

71

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