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WindPRO / PARK - EMD International AS.

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Introduction to the N.O. Jensen Wake Model<br />

Single w ake w ind speeds [m/s]<br />

Radial distance [m]<br />

300<br />

250<br />

200<br />

150<br />

100<br />

50<br />

0<br />

-50<br />

-100<br />

-150<br />

-200<br />

-250<br />

-300<br />

0<br />

200<br />

400<br />

600<br />

Dow nstream distance [m]<br />

800<br />

1 000<br />

1 200<br />

10<br />

9.834<br />

9.669<br />

9.503<br />

9.338<br />

9.172<br />

9.006<br />

8.841<br />

8.675<br />

8.509<br />

8.344<br />

8.178<br />

8.013<br />

7.847<br />

7.681<br />

7.516<br />

7.35<br />

7.185<br />

7.019<br />

6.853<br />

6.688<br />

6.522<br />

6.356<br />

6.191<br />

6.025<br />

5.86<br />

5.694<br />

5.528<br />

5.363<br />

5.197<br />

5.032<br />

4.866<br />

4.7<br />

Figure 2: N.O. Jensen wake model - wake development after a single turbine.<br />

Multiple Wake Calculation<br />

Katic et al. [1] suggests, that multiple wakes are calculated through the ‘sum of squares of velocity deficits’<br />

wake combination model. Thus, the N.O. Jensen model initially implemented in the <strong>WindPRO</strong> <strong>PARK</strong><br />

module as well as the WAsP / Park module uses the sum of squares of velocity deficit to calculate a<br />

combined wake contribution. The combined effects of multiple wakes are found as:<br />

δV<br />

n<br />

n−1<br />

= ∑ kn<br />

k = 1<br />

( ) 2<br />

δV<br />

This model is treated in a succeeding chapter.<br />

References<br />

[1]I. Katić, J. Højstrup & N.O. Jensen, A Simple Model for Cluster Efficiency, European Wind Energy<br />

Association, Conference and Exhibition, 7-9 October 1986, Rome, Italy.<br />

Page 2-2

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