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96 H. Kantz et al.<br />

# of occurences per day<br />

100000<br />

10000<br />

1000<br />

100<br />

10<br />

day 191<br />

1<br />

0 1 2 3 4 5 6 7<br />

increase of wind speed during 2 s [m/s]<br />

Fig. 16.3. The distribution of wind gusts for different days. Results shown below<br />

are obtained for the gusty day 191<br />

against changes of this interval. The histograms of these gust strengthes<br />

show approximately an exponential distribution (Fig. 16.3). The previously<br />

discussed prediction schemes are not suitable to predict strong gusts, i.e. a<br />

coming gust does typically not cause a large positive difference between predicted<br />

and actual value, ˆvt+k − vt (the persistence predictor trivially predicts<br />

this difference to be 0). However, the Markov chain approach offers a probabilistic<br />

way of forecasting: One can extract, for every time instance, a probability<br />

of a gust to come. This is done by straightforwardly interpreting the<br />

conditional probability densities of the Markov chain or evident variants of<br />

these. In order to estimate the probability of a gust to happen during the<br />

following 2 s, one selects all data segments at past times lvt + g, i.e. which fulfil our gust criterion,<br />

gives the actual probability of a gust of strength g to come.<br />

This is a probabilistic prediction scheme, and despite a large predicted<br />

probability no gust might follow. This illustrates the difficulty of verification:<br />

The prediction scheme yields a probability, the actual observation will yield<br />

a yes/no result. In order to check the predicted probabilities, we apply the<br />

technique of the reliability plot: We create sub-samples of data for which the<br />

predicted gust probabilities are in some small interval pgust(t) ∈ [r − ∆r, r +<br />

∆r]. If the predicted probabilities are without any bias, then the relative<br />

number of gust events inside such a sample should be in good agreement with<br />

r (for sufficiently small ∆r). Indeed for r smaller than 1/2 this property is

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