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This method gives a good accuracy (about 0.5 K for accuracy of brightness temperature<br />

measurement better than 0.1 K) but sometimes results are not stable.<br />

A more stable solution, having approximately the same accuracy, is given by a second<br />

method, which uses a variation of linear statistical retrieval (Turchin, 1967; Westwater et al.,<br />

1998). To implement this algorithm, it was constructed a covariance matrix which describes<br />

the brightness temperature differences at equally spaced zenith angles ranging from 0 to<br />

90 ◦ with the in situ temperature. After having performed an eigenvector analysis on this<br />

covariance matrix a stable solution of the inverse problem is achieved. Other more modern<br />

frequently used method in radiometry include neural network in<strong>version</strong> and Kalman filtering.<br />

A complete work on the most part of possible in<strong>version</strong> methods is given in Janssen (1993).<br />

14.5 An angular scanning temperature profile radiometer<br />

A commercial example of an angular scanning temperature profiler radiometer is shown in<br />

Fig. 181 and was produced by the Russian scientific company ATTEX in cooperation with<br />

the Dutch company Kipp & Zonen: a polar regions <strong>version</strong> of the radiometer was realized<br />

in 2001 with improved vertical resolution and was called MTP-5P (P stands for polar). The<br />

MTP-5P has a microwave radiometer with the center frequency at about 60 GHz which<br />

measures the radio brightness temperature of the atmosphere with a high sensitivity (0.04 K<br />

at 1 s of integration time) at different discrete elevation angles. On the base of this discrete<br />

measurement, it is always possible to retrieve the discrete atmospheric temperature profile<br />

from the ground level around 5 m until to 600m(instrument’s intrinsic superiorlimit) with an<br />

accuracy 0.5 K at a vertical resolution at lowerquotas of 10–20 m. The MTP-5P’s electronics<br />

and parabolic antenna – beam aperture width of 0.5degrees – are housed into a thermostatic<br />

trailer (see Figure 182) whose temperature is controlled to within 5 K: over a year’s time, the<br />

internal radiometer’s receiver temperature should vary by less than 1 K.<br />

Figure 181: Meteorological temperature profiler (polar <strong>version</strong>) MTP- 5P<br />

Internal calibration of the instrument is achieved by sequentially switching between the antenna<br />

and a reference blackbody’s radiation source (as a current controlled resistive dummy).<br />

The complete radiometer’s technical specifications are reported in Table 20.<br />

The brightness temperature data Tb(θ) for an angular scanning, MTP-5 radiometer has the<br />

previousintegral form ofEq. (347)where atmosphericmolecularoxygenabsorptioncoefficient<br />

in weighted function W ν0 (z,θ) was calculated from Rosenkranz (1992) and upper limit of<br />

integration is H = 1 km. The statistical a priori database used for the setting up of the<br />

in<strong>version</strong> process was a 2-year dataset of radiosonde’s temperature profiles data from Russian<br />

upperairstationnetwork.Innormaloperationtemperature profilesT(z)are typicallyprovided<br />

every 3 min.<br />

Calibration factors require infrequent updating, perhaps once a year. External calibration<br />

<strong>DTU</strong> Wind Energy-E-Report-0029(EN) 269

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