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ESA Document - Emits - ESA

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HMM<br />

Assessment Study<br />

Report: CDF-20(A)<br />

February 2004<br />

page 243 of 422<br />

3.4.3.4.3 Regenerative and thermoelectric coolers<br />

These systems are not considered for such volume (above 10 m3) being poorly efficient when<br />

high refrigeration loads are required in the case of regenerative system (Stirling for example), or<br />

to low temperatures with thermo-electric cooling (above 140K).<br />

3.4.3.4.4 Recuperative coolers<br />

Among possible recuperative systems, the Turbo-Brayton (TB) cycle presents a relatively high<br />

thermodynamic efficiency at 20K and appears to be a good candidate today for this range of<br />

cooling power (5-15W). Available for ground applications (100 watts, 4K), the challenge is to<br />

downsize the cooling power and miniaturize elements to fit space-related requirements, which<br />

was done in particular for NICMOS (5W@65K) and MELFI projects (47Wat190K).<br />

Developments are ongoing in U.S. and in Europe (<strong>ESA</strong> TRP on a compressor 50mWat6K, 300W<br />

input power).<br />

Expected efficiency of a TB is about 10 to 15% Carnot at 35K today (an equivalent efficiency<br />

can be reasonably projected in the coming years for 20K), which would require an input power<br />

of the order of 950W.<br />

Figure 3-79: COP efficiency and input power as function of Tc<br />

A higher boiling temperature allows significant reduction of the cooler input power: having a<br />

subcritical liquid reduces input power by 55%. The primary objective however is densification of<br />

the hydrogen to reduce the total amount at launch. Increasing the fluid temperature is therefore<br />

secondary and only possible if the launcher capability on the volume is reached.<br />

Figure 3-80: TB schematic (1 stage)

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