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46 E. Bibor and C. Masson<br />

% error (Psect - Pgen) / Pgen<br />

15<br />

10<br />

5<br />

0<br />

−5<br />

−10<br />

−15<br />

4<br />

5 6 7 8 9 10<br />

V ∞ - bins of 0.5(m/s)<br />

11 12<br />

Fig. 8.2. Comparison between correlations by sectors and general correlation for<br />

all valid sectors on power curves<br />

(a) (b)<br />

V ∞ (m/s)<br />

20<br />

18<br />

16<br />

14<br />

12<br />

10<br />

8<br />

6<br />

4<br />

2<br />

0<br />

0<br />

+<br />

+<br />

+<br />

+<br />

2 4 6<br />

+<br />

+<br />

+<br />

+<br />

+<br />

+<br />

+<br />

+<br />

+<br />

+<br />

+<br />

+<br />

8 10 12 14 16 18 20 22<br />

V nac (m/s)<br />

+<br />

+<br />

+<br />

+<br />

+<br />

+<br />

+<br />

Experimental: general<br />

correlation<br />

Numerical - without U<br />

Numerical - with U1<br />

Numerical - with U2<br />

Fig. 8.3. (a) Attachment unit on the nacelle (b) Influence of the attachment unit<br />

positions, U1 and U2, distant of 50 cm, have been analysed (Fig. 8.3b). The<br />

influence of the U-beam is significant, and can explain in part the differences<br />

observed between the numerical and experimental correlations.<br />

8.6 Conclusion<br />

Three main conclusions were drawn from experimental and numerical analysis.<br />

First, using the correlation provided by the manufacturer for any type of<br />

terrain can lead to important error. The second conclusion is that the use of<br />

a general correlation for all the valid sectors is not a bad practice. Finally,<br />

it has been numerically proven that for this WT, the attachment unit of the<br />

nacelle anemometer is an important cause of the flow perturbation.

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