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Coherence<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

10 −3<br />

Geometry Errors, r = 41 m<br />

10 −2<br />

10 −1<br />

Frequency (Hz)<br />

10 0<br />

d = 30 m<br />

d = 60 m<br />

d = 90 m<br />

d = 120 m<br />

d = 150 m<br />

Figure 141: Measurement coherence for a hub-mounted lidar with a scan radius of 41 m at<br />

five different preview distances. Only geometry errors are included.<br />

Coherence<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

10 −3<br />

10 −2<br />

Wind Evolution, r = 41 m<br />

10 −1<br />

Frequency (Hz)<br />

10 0<br />

d = 30 m<br />

d = 60 m<br />

d = 90 m<br />

d = 120 m<br />

d = 150 m<br />

Figure 142: Measurement coherence for a hub-mounted lidar with a scan radius of 41 m at<br />

five different preview distances. Only wind evolution errors are included.<br />

10.5.3 Wind Evolution<br />

A major source of preview measurement error is the evolution of the turbulence between<br />

the time it is measured by the lidar and the time it appears at the turbine rotor as a wind<br />

disturbance. While for a fixed scan radius r, measurement errors due to the measurement<br />

geometry decrease as preview distance increases, errors due to wind evolution become more<br />

severe, since there is additional time for the turbulence to evolve.<br />

Wind evolution can be described by a coherence function between wind speeds at two<br />

points separated in the longitudinal (along-wind) direction. A popular longitudinal coherence<br />

formula used in the wind turbine control community (Bossanyi et al. 2012b; Schlipf et al.<br />

2012a; Laks et al. 2013) is presented in Kristensen (1979). The Kristensen coherence formula<br />

is a function of frequency, longitudinal separation, mean wind speed, turbulent kinetic energy,<br />

and a turbulence length scale. Wind evolution becomes more severe when longitudinal separation<br />

or turbulent kinetic energy are increased and becomes less severe as mean wind speed<br />

increases. Longitudinal coherence curves using the Kristensen (1979) formula are shown in<br />

Fig. 142 for several preview distances. A mean wind speed of 13 m/s is used with a turbulence<br />

intensity of 10%. Wind evolution tends to affect high frequencies more than low frequencies<br />

and, as a result, very low-frequencystructures in the wind do not change significantlybetween<br />

the measurement point and the turbine.<br />

The IEC von Karman wind model used in this chapter only defines spatial coherence in<br />

the transverse and vertical (yz) plane. This model assumes that wind speeds are perfectly<br />

<strong>DTU</strong> Wind Energy-E-Report-0029(EN) 205

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