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174 E. Anahua et al.<br />

Elec. Power Output [kW]<br />

3000<br />

2500<br />

2000<br />

1500<br />

1000<br />

500<br />

0 0 5 10 15 20 25 30 35<br />

<strong>Wind</strong> speed [m/s]<br />

Fig. 31.1. Typical nonlinearity effects on measured power output data of a WEC<br />

of 2 MW [5]. A complex behaviour is observed by the dynamics response on sudden<br />

changes of wind velocity. The dots are instantaneous measured data and the solid<br />

line is the average power output 〈L(u)〉<br />

around 〈u〉, i.e. small turbulent intensities ti = σu/〈u〉. It is known that<br />

the wind fluctuation distribution presents an anomalous statistics around the<br />

mean value [1], therefore this is again limited. As an improvement, this article<br />

reports that the dynamical behaviour of the power output of a WEC, which<br />

acts as an attractor, can be described by a simple function of relaxation and<br />

noise. We have shown that those two parts describe the power curve properly if<br />

they are calculated from stationary wind measurements. This analysis is very<br />

usefull to describe power curve characteristics for situation with increased<br />

turbulent intensities and it can be easily applied to measured data.<br />

31.2 Simple Relaxation Model<br />

The instantaneous elect. power output of a WEC defined by: L(t) =Lfix(u)<br />

+ ℓ(t) can be described by the following relaxation model [2], see also [6]<br />

ℓ(t) ∝ e| −αt<br />

d<br />

L(t) =−αℓ(t)+g(L, t)Γ (t),<br />

dt

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