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36 Helicopter Aerodynamics with Emphasis Placed on Dynamic Stall 201<br />

Dynamic Stall Vortex During Up-stroke Motion of NACA 0012 Airfoil<br />

Left Figure: α = 21�, Right Figure: α = 25�<br />

Figures Include Instantaneous Streamlines and Singular Points<br />

Fig. 36.2. Vorticity contours at two time-instants during up-stroke<br />

damping. If these loops are travelled in anti-clockwise sense, the situation is<br />

stable, i.e. energy is shifted from the blade into the surrounding fluid. However<br />

if the loop is traversed in the clockwise sense (see indication in Fig. 36.2) an<br />

unstable flow condition occurs and energy is transferred from the flow to the<br />

blade structure. This is a critical situation insofar as dangerous stall flutter<br />

may occur.<br />

Figure 36.2 shows the calculated details of the vorticals flow at two instants<br />

of time during the up-stroke motion. In the left figure the vortex has just been<br />

created close to the blade leading edge, has started to travel along the upper<br />

surface but is still attached to the surface. In this phase the vortex creates<br />

extra lift (see Fig. 36.1). Very short time later (right sequence of Fig. 36.2)<br />

the vortex has been lifted off the blade surface, stall has been started and negative<br />

vorticity is created at the blade trailing edge moving forward underneath<br />

the Dynamic Stall Vortex. In this phase the complex flow phenomenon occur<br />

which cause the strong decay of lift and creation of negative aerodynamic<br />

damping.<br />

36.3 Numerical and Experimental Results<br />

for the Typical Helicopter Airfoil OA209<br />

In October 2004 DLR has done experiments in the DNW-TWG wind tunnel<br />

facility located at the DLR-Centre in Göttingen. These tests are part of the<br />

DLR/ONERA joint project “Dynamic Stall.” Within this project it was decided<br />

to use the OA209 (9% thickness) airfoil section as the standard airfoil.<br />

The OA209 airfoil is in use on a variety of flying helicopters. Measurements<br />

on a 0.3 m chord and 1 m span blade model (extended between wind tunnel<br />

side-walls) have been carried out. The objectives of these almost full size tests<br />

have been to study the details of the dynamic stall process by both numerical

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