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Figure186:Temperaturebehaviour(topfigure)andtemperaturecrosssection(bottomfigure)<br />

during the all field experiment (18 November 2002 to 15 December 2002)<br />

shown in Fig. 185, multi channel method without scanning had a low vertical resolution at<br />

the lowest part of the ABL (about 300 m).<br />

Thesecondmethod(ourdiscussedcasestudy) isbasedonusinganangular-scanningsinglechannel<br />

radiometer with the central frequency of 60 GHz. This method and the instrument<br />

were proposed by Troitsky et al. (1993) and discussed in detail by Kadygrov and Pick (1998)<br />

and Westwater et al. (1999).<br />

Due to the large atmospheric absorption by molecular oxygen at 60 GHz, angular-scanning<br />

method has some advantages for ABL temperature profiling over the multi channel method<br />

(Kadygrov et al., 2004a), which can be summarized as follows:<br />

• it can really to operate in all weather conditions: the measurements do not depends on<br />

changes of water vapor density or on the presence of fog or low clouds<br />

• better vertical resolution in the lower 300 m<br />

• the bandwidth of the receiver is very wide which provides a high sensitivityof the receiver<br />

(about 0.04 K at 1 s integration time);<br />

• instrument has a small sizes, is very portable, can provide reliable automated continuous<br />

profiling from a variety of sites and relatively small cost<br />

However single-channel angular-scanning method, how we have seen, has its limitations in<br />

altitude measurement. It can measures only from the ground level up to 1000 m.<br />

Notation<br />

Aν fraction of incident energy absorbed from a direction<br />

Bν(T) brightness<br />

c vacuum speed of light<br />

dIν variation of specific intensity<br />

ds elementary segment in the direction of propagation<br />

dΩ solid angle element<br />

h Planck’s constant<br />

altitude<br />

Hb boundary-layer height<br />

Iν specific intensity<br />

k Boltzmann’s constant<br />

MPM microwave propagation model<br />

RTE radiative transfer equation<br />

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

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