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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.

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