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ESA Document - Emits - ESA

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s<br />

flux [W/m2]<br />

250<br />

200<br />

150<br />

100<br />

50<br />

0<br />

energy on 2 face radiator (alp=0.2, eps=0.8)<br />

rad.<br />

0 15 30 45 60 75 90 105 120 135 150 165 180<br />

angle (normal rad. to center planet) [deg.]<br />

receiv ed inf rared receiv ed albedo (sun coplanar to rad.) absorbed total<br />

Radiator area [m2]<br />

2 faces WP radiator (eff. 0.8), biphasic, P=12kW<br />

HMM<br />

Assessment Study<br />

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

February 2004<br />

page 177 of 422<br />

100<br />

90<br />

80<br />

70<br />

60<br />

50<br />

40<br />

1 face radiato r (no heat load, other face adiabatic)<br />

2 face radiato r<br />

(no heat load)<br />

30<br />

20<br />

10<br />

0<br />

-60 -40 -20 0 20 40 60 80 100 120<br />

temp. fluid [C]<br />

0 30 60 90 deg.<br />

Figure 3-36: Total energy on radiator (L), Radiator size versus angle and temp. fluid (R)<br />

Figure 3-36 (L) shows the total absorbed energy from Earth as a function of the angle it normal<br />

makes with the centre of the planet (the Sun being considered in the radiator plane) Figure 3-36<br />

(R) shows the impact of this parasitic heat load on the radiator size. Despite planetary heat loads<br />

and the prize of the rotation angle, the size of a two-face radiator design remains inferior to a<br />

single-face (as long the radiator temperature remains superior to the planet temperature). The<br />

cost of a full tolerance of planetary heat load decreases with the fluid temperature increase (at<br />

5C, the ratio is 1.17). The option of a fixed radiator could be therefore tolerated at this expense<br />

and with an adequate spacecraft attitude (no Sun on the radiators).<br />

The technology to rotate a biphasic radiator is not available in Europe (nor is there a<br />

development plan), so a fixed radiator is retained with an adequate tolerance to planetary heat<br />

loads.<br />

Out of the influence of the planet, the system performs optimally and the heat rejection<br />

capability is naturally increased (by a ratio 1.37). The flexibility of the secondary loop is<br />

provided by the bypass valve regulating the mass flow and therefore the sink temperature<br />

provided to the users.<br />

The minimum set point (high heat load) for the primary loop is set to 4/7C (inlet 13/18C), which<br />

gives a minimum of 0/4C required from the secondary loop inlet at the heat exchanger level.<br />

Setting the bypass inlet at -5/-1C provides a possible solution, and drives a radiator area of 56.6<br />

m 2 .<br />

The Lockheed-Martin PVR assembly mounted on the ISS truss is taken as a baseline (see last<br />

picture in Table 3-26). The following configuration is chosen: 8 panels, each 2.1 x 3.4 m 2 ,<br />

deployable by an electric motor ‘scissor’ mechanism. Total weight is 849 kg per assembly (x 2).<br />

White paint coating (type PSG121FD) is applied on both sides. Its degradation over time is well<br />

known and can be controlled through a careful illumination from solar UV.<br />

Two identical systems are mounted symmetrically on the spacecraft body.<br />

3.3.3.4.5 Insulating system and thermal protection<br />

sun

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