Jahresbericht 08 - PMOD/WRC
Jahresbericht 08 - PMOD/WRC
Jahresbericht 08 - PMOD/WRC
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14<br />
Instrument Development<br />
Monitor to Determine the Integrated Transmittance of Windows (MITRA)<br />
and the Cryogenic Solar Absolute Radiometer (CSAR)<br />
André Fehlmann, Wolfgang Finsterle, and Werner Schmutz in collaboration with Ulrich Straumann, University of Zürich,<br />
Peter Blattner, METAS, Rainer Winkler, Eric Usadi, David Gibbs, and Nigel Fox, NPL, England<br />
We report on the nearly finished CSAR design phase<br />
and the prototype status of MITRA.<br />
The <strong>PMOD</strong>/<strong>WRC</strong>, METAS and NPL project (Fehlmann,<br />
20<strong>08</strong>) to build a cryogenic solar absolute radiometer is progressing<br />
well. During the last year the CSAR design was<br />
further refined. Hardware components such as the cryogenic<br />
cooler have been selected and ordered. Currently,<br />
detailed drawings of the instrument are being finalized at<br />
NPL in London. In April 2009 METAS (Bern, Switzerland)<br />
will then start to produce the CSAR parts which we then<br />
plan to assemble in July 2009. Figure 1 shows a drawing<br />
of the CSAR instrument.<br />
Figure 1. The CSAR instrument without vacuum tank. The dark gray part<br />
on the left is the cryogenic cooler which allows the instrument to be cooled<br />
to 20 Kelvin.<br />
Development of MITRA<br />
The monitor to determine the integrated transmittance of<br />
windows has already reached prototype status (Figure 2).<br />
MITRA has two identical cavities which are mounted on a<br />
common heat sink via two thermal resistors. Thermopiles<br />
form these resistances and simultaneously measure the<br />
temperature differences between the cavities and the heatsink.<br />
Since these temperature differences are proportional<br />
to the solar irradiance and both cavities see the same sun,<br />
we end up with a constant ratio of the two signals produced<br />
by the thermopiles.<br />
Characterization of MITRA<br />
Experiments with MITRA in the laboratory revealed a nonconstant<br />
ratio of the thermopile signals with changing irradiance.<br />
This is due to thermal relaxation time constants that<br />
are not equal for both cavities. We managed to fine-tune<br />
the thermal resistances and thermal capacities of the instrument<br />
to obtain a constant signal at all times.<br />
Once MITRA has proven itself in ground-based solar measurements<br />
we will start to measure the transmittance of our<br />
Sapphire and Quartz windows. These windows have been<br />
characterized at METAS in the 300-1000 nm wavelength<br />
range and will be characterized at <strong>PMOD</strong>/<strong>WRC</strong> in the 250-<br />
500 nm and 1000-5000 nm ranges.<br />
As soon as the final CSAR design is fixed, we will start to<br />
develop the definitive MITRA instrument. In doing so, special<br />
attention will be payed so that both instruments have<br />
the same optical setup, i.e. baffles, apertures and geometries.<br />
Thus, the problem of stray light, which is to be characterized,<br />
will be similar for both instruments and will not<br />
unintentionally introduce a systematic effect.<br />
Figure 2. The dual cavity monitor MITRA prototype. Not shown is<br />
the instrument housing which acts as a wind-shield and thus makes<br />
it insensitive to ambient temperature.<br />
References: Fehlmann A., Finsterle W., Schmutz W., Straumann U.,<br />
Blattner P., Winkler R., Gibbs D., Fox N., 20<strong>08</strong>,<br />
Cryogenic Solar Absolute Radiometer (CSAR),<br />
<strong>PMOD</strong>/<strong>WRC</strong> Annual Report 2007.