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may be calculated from the two Weibull parameters, the scale parameter A and the shape<br />

parameter k, using the gamma function Γ, and the air density ρ (≈ 1.245kgm−3 at 10◦C) as<br />

E = 1<br />

2 ρA3 <br />

Γ 1+ 3<br />

<br />

(350)<br />

k<br />

The uncertainties for the four parameters; mean wind speed, Weibull A and k, and energy<br />

density can be calculated in S-WAsP. The uncertainty calculation estimates the difference of<br />

the Weibull A and k fitted function and the measured wind distribution based on the available<br />

number of samples. We follow the equations from the appendix in (Pryor et al., 2004). We<br />

assume that each SAR-based wind map is accurate and that the influence of time sampling<br />

is insignificant to the estimates. In other words, we assume the diurnal wind pattern to be<br />

described accurately using morning and evening observations only.<br />

Studies from the North Sea and Baltic Sea have shown SAR wind maps to be a useful/valuable<br />

source of information for the estimation of Weibull A and k (Badger et al.,<br />

2010a; Christiansen et al., 2006; Hasager et al., 2011a).<br />

15.11 The wind class method<br />

Envisat ASAR and ERS-1/2 SAR scenes are nowadays freely available in large quantities<br />

over Europe. In earlier times there were limitations. For commercial application a relatively<br />

high cost was associated. This prompted a need for an alternative SAR-based wind resource<br />

method in S-WAsP: the wind class method (Badger et al., 2010a). The method is based<br />

on representative selected sampling of 135 SAR scenes each with wind conditions similar to<br />

representative long-term wind conditions as evaluated from the global atmospheric model<br />

results from NCAR NCEP re-analysis. Thus the first processing step is to evaluate the longterm<br />

statistics from large-scale models and assess the weighting function for the selected<br />

representative wind conditions. This method is also used in the KAMM/WAsP wind atlas<br />

methodology (Frank et al., 2001). The second step is to distribute the SAR scenes amongst<br />

the wind classes based on look-up tables with the specific dates and times when each given<br />

wind situation occurs. The third step is to retrieve and process the SAR scenes to wind fields.<br />

The fourth and final step is to use the relevant weighting functions from the first step to<br />

produce representative SAR-based wind resource statistics from the series of SAR wind fields.<br />

The final results are maps of Weibull A and k, mean wind speed and energy density. The<br />

method was used in United Arab Emirates and compared well with mesoscale model results<br />

(Badger et al., 2010b). Figure 193 shows the mean wind speed at 10 m over the United Arab<br />

Emirates.<br />

Figure 193: 10 m mean wind speed maps over the United Arab Emirates from (left) Envisat<br />

ASAR wind fields and (right) KAMM mesoscale modeling. From Badger et al. (2010b).<br />

The wind class method was evaluated in the North Sea using in-situ data for comparison.<br />

Theresultswereverygood.Theoverallagreementwithmastobservationsofthewindresource<br />

was within±5% for mean wind speed and Weibull scale parameterand within ±7% forenergy<br />

density and Weibull shape parameter. Similar results were obtained from using more than<br />

288 <strong>DTU</strong> Wind Energy-E-Report-0029(EN)

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