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4.5 Ground based, vertical scan configuration wind field<br />

parameter determination<br />

4.5.1 Least-squares fitting routine<br />

The data that are fed to the fitting routine consist of up to 150 pairs of values of 〈VLOS〉 and<br />

azimuth angle φ. In conditions of uniform wind flow, this gives rise to a rectified cosine wave<br />

of the form:<br />

〈VLOS〉 = |acos(φ−b)+c|. (100)<br />

Thederivationofthisfunctionisstraightforwardandcanbefoundinanumberofpublications,<br />

e.g. Banakh et al. (1993). The peaks of the function correspond to the azimuth angle aligned<br />

parallel or anti-parallel to the wind direction. The function passes through zero when the<br />

azimuth angle is perpendicular to wind bearing since there is no component of velocity along<br />

the line of sight. The data are also conveniently displayed on a polar plot (Figure 46), which<br />

provides information at a glance on the speed, direction and vertical wind component. A<br />

standard least-squares fitting routine provides the best estimates of the values of the three<br />

floating parameters (a, b and c).<br />

Figure 46: Wind lidar output for a ground-based, vertical scan ZephIR, illustrating many of<br />

the features of a wind profile measurement. This example has been obtained at a height<br />

150 m above ground level, one of several heights being probed in sequence. The lower trace<br />

shows 147 individual line-of-sightwind speed values, obtained over a total period of 3 seconds<br />

(plotted as white squares against azimuth scan angle). The same data, along with the leastsquares<br />

fit in red, are displayed above in polar coordinates on the figure-of-eight plot showing<br />

the wind bearing to lie slightly to the East of North. The wind parameters, derived from the<br />

fit, appear in the table on the right; the horizontal wind speed at this height is determined<br />

to be 9.1 m s −1 . The plot on the upper left shows one of the spectra from which each point<br />

on the other graphs is derived.<br />

The high level of redundancy in the fitting process is advantageous and can be used to<br />

identify non-uniform flow. The root mean square deviation of the points from the optimum<br />

solution gives an indication of the quality of fit, and this can be related to the value of<br />

turbulent kinetic energy (TKE; see Wagner et al. (2009)). More work is needed to establish<br />

a full understanding of the turbulence information available from lidar signals (Banakh et al.,<br />

1999). Note that information on turbulence is also available from the spectral widths of the<br />

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

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