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Boundary-layer height detection with a ceilometer at a coastal ... - Orbit

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3 Site and measurements<br />

In this section the site loc<strong>at</strong>ion is presented and some of the instruments used there. The<br />

theoretical background of the <strong>ceilometer</strong>, wind lidar and sonic anemometer measurements is<br />

explained, along <strong>with</strong> a present<strong>at</strong>ion of the available d<strong>at</strong>a from the site d<strong>at</strong>abase.<br />

3.1 Høvsøre<br />

Høvsøre is a farm area loc<strong>at</strong>ed <strong>at</strong> the westcoast of Jutland, seen in Figure 5(a). Here, a<br />

<strong>ceilometer</strong> has oper<strong>at</strong>ed almost continuously since january 2007. The loc<strong>at</strong>ion of Høvsøre was<br />

chosen in 2002 to be a n<strong>at</strong>ional test facility for large wind turbines, seen in Figure 5(b). Due<br />

to the loc<strong>at</strong>ion and the type of terrain, wind speeds are very high 4 and general wind p<strong>at</strong>terns<br />

are very well understood, providing excellent conditions for the testing (Høvsøre infofolder,<br />

2013).<br />

5 ◦ E 7 ◦ E 9 ◦ E 11 ◦ E 13 ◦ E<br />

NORTH SEA<br />

Høvsøre<br />

DENMARK<br />

56 ◦ N 56 ◦ N<br />

Copenhagen<br />

km<br />

0 50 100<br />

7 ◦ E 9 ◦ E 11 ◦ E 13 ◦ E<br />

(a)<br />

(b)<br />

Figure 5: (a): Map of Jutland, <strong>with</strong> Høvsøre indic<strong>at</strong>ed (map made by Rogier Floors). (b):<br />

View of Høvsøre test st<strong>at</strong>ion, <strong>with</strong> oper<strong>at</strong>ional wind turbines. Picture from Høvsøre infofolder<br />

(2013).<br />

3.2 The <strong>ceilometer</strong><br />

The <strong>ceilometer</strong> is a single lens LIDAR (Light Detection And Ranging) device, which is primarily<br />

used to detect cloud base and vertical visibility. It transmits short pulses of light in the<br />

near-vertical direction. The light is sc<strong>at</strong>tered by particles in the air, aerosols, cloud droplets<br />

and precipit<strong>at</strong>ion. The returned light is then collected in a receiver inside the <strong>ceilometer</strong><br />

(Vaisala User’s Guide, 2004). The <strong>height</strong> h from which the returned signal comes from may<br />

be estim<strong>at</strong>ed as<br />

h = ct<br />

(14)<br />

2<br />

where c is the speed of light and t the time delay. As the speed of light is taken as a constant,<br />

the <strong>height</strong> may be calcul<strong>at</strong>ed directly from the time delay. The signal strength as a<br />

4 the annual mean wind speed is ∼9.3 m/s <strong>at</strong> 80 m<br />

16

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