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118 S. Barth et al.<br />

p(u τ) [a.u.]<br />

10 −4<br />

10 −2<br />

10 −4<br />

10 −6<br />

10 −8<br />

10<br />

−10 0 10<br />

−8<br />

10<br />

uτ /στ −12<br />

10 −10<br />

p(u τ) [a.u.]<br />

−10 0<br />

uτ/στ 10<br />

Fig. 20.3. Atmospheric PDFs: Symbols represent the normalized PDFs of the<br />

atmospheric data sets. Straight lines correspond to a fit of distributions according to<br />

(20.4). All graphs are vertically shifted against each other for clarity of presentation.<br />

Left: sonic anemometer: From top to bottom τ takes the values: 0.5s, 2.5s, 25s,<br />

250 s and 4, 000 s. Right: hotwire anemometer: From top to bottom τ takes the<br />

values: 2 ms, 20 ms, 200 ms and 2, 000 ms<br />

hot-wire anemometer in an atmospheric flow during a period of stationary<br />

mean wind speed. In both cases the scale dependent statistics can be described<br />

with 20.4.<br />

20.3 Conclusions and Outlook<br />

Atmospheric velocity increments and their occurrence statistics are related<br />

to loads on wind turbines. For constructing wind turbines a model that<br />

reproduces the right increment distributions for every location should therefore<br />

be used. Our approach is a good candidate to achieve such a robust model.<br />

References<br />

1. U. Frisch: Turbulence. The Legacy of A.N. Kolmogorov, Cambridge University<br />

Press, Cambridge, 1995<br />

2. B. Castaing, Y. Gagne, E.J. Hopfinger: Physica D 46, 177, 1990<br />

3. T. Burton, D. Sharpe, N. Jenkins and E. Bossanyi: <strong>Wind</strong> <strong>Energy</strong> Handbook,<br />

Wiley, New York, 2001

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