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262 S. Ivanell et al.<br />

Assuming that all wake vorticity is included in the tip and the root vortex,<br />

the circulation at tip and root should approximately correspond to the maximum<br />

bound circulation of the blade. This is of course an idealization, since<br />

the roll-up of the vortex sheets is expected to form a concentrated vorticity<br />

distribution in the far wake [7]. The computed circulation at the blades is<br />

given in Fig. 48.3.<br />

Figure 48.3 shows some wiggles that start at about 500 ◦ behind the blades<br />

for the root vortex and about 800 ◦ behind the blade for the tip vortex. These<br />

are most likely due to integration errors when integrating the circulation.<br />

At these positions the vortex core starts to be smeared out and it therefore<br />

becomes difficult to identify a good integration path.<br />

The results, however, correspond fairly well to classical theories from<br />

Helmholtz. The tip vortex leaves the blade with a circulation value close to<br />

the maximum bound circulation at the blades. The root vortex leaves the<br />

blade with a much lower value of the circulation, but it increases rapidly and<br />

reaches values at the same order as the bound circulation. The reason why<br />

the root vortex is smeared out earlier than the tip vortex is partly because the<br />

vortex cores are closer at the root and partly because of the radial gradient of<br />

the circulation. The result is in good agreement with classical theorems from<br />

Helmholtz, from which it follows that the wake tip vortex has the same circulation<br />

as the maximum value of the bound circulation on the blade. A likely<br />

explanation for this good agreement is that the symmetry of the flow domain<br />

prohibits the roll-up of the vortex sheet from the blades.<br />

Circulation<br />

0.14<br />

0.13<br />

0.12<br />

0.11<br />

0.1<br />

0.09<br />

0.08<br />

0.07<br />

0.06<br />

0.05<br />

96 Tip,eps =1 Re1<br />

96 Tip,eps =1 Re2<br />

96 Tip,eps =1 Re3<br />

96 Rot,eps =1 Re1<br />

96 Rot,eps =1 Re2<br />

96 Rot,eps =1 Re3<br />

Maximum circulation at blade<br />

0 200 400 600 800 1000 1200<br />

Deg. behind blade<br />

Fig. 48.3. The figure shows the circulation distribution in the wake at three different<br />

Reynolds number compared with the maximum circulation at the blade [8]

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