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Master Thesis - OUFTI-1

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The last property to determine is the value of the resistance. Thermal simulations<br />

performed last year [12] allow to determine that the power necessary to heat the batteries, is<br />

250 mW . Assuming that heaters are supplied by a tension of 2.5 V (which is a conservative<br />

approach because the tension of the batteries can not pass under 2.7 V ), the resistance<br />

can be easily calculated (see Equation 3.7.1).<br />

P = U I = U 2<br />

R ⇒ R = U 2<br />

P = 2.52 = 25 Ω (3.7.1)<br />

0.25<br />

The available heater that is closest to this value is a heater with a resistance of 23.7 Ω,<br />

which is again a conservative approach because the power generated will be higher than<br />

250 mW .<br />

The heaters will be glued, as already mentioned, directly on the batteries, on their face<br />

+Z (which corresponds to the side of the box).<br />

3.7.2 Heaters' control system<br />

Two solutions were investigated to realize the heaters' control system:<br />

• Creation of an electrical circuit that used heat sensors to decide when the heaters<br />

have to be supplied.<br />

• A thermostat that is self-ecient.<br />

In accordance with the KISS philosophy, the second solution was preferred because it<br />

is more reliable.<br />

The selected thermostats are Klixon 4BT − 2 [42], illustrated in Figure 3.11 (the dimensions<br />

are given in inches).<br />

Figure 3.11: Thermostat Klixon 4BT − 2<br />

56

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