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BULETINUL INSTITUTULUI POLITEHNIC DIN IAŞI

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112 Vlad Marţian et al<br />

Current Intensity [A]<br />

80<br />

70<br />

4.5<br />

4<br />

60<br />

3.5<br />

50<br />

3<br />

2.5<br />

40<br />

2<br />

30<br />

1.5<br />

20<br />

1<br />

10<br />

0.5<br />

0<br />

0<br />

0 10 20 30 40 50 60 70<br />

Time [min]<br />

Battery Voltage [V]<br />

Current Intensity Battery Voltage<br />

Fig. 8 – Current intensity and voltage.<br />

Eoc [V]<br />

4<br />

3.5<br />

3<br />

2.5<br />

2<br />

1.5<br />

1<br />

0.5<br />

0<br />

0<br />

0 0.2 0.4 0.6 0.8 1 1.2<br />

0.09<br />

0.08<br />

0.07<br />

0.06<br />

0.05<br />

0.04<br />

Rint [Ω]<br />

0.03<br />

0.02<br />

0.01<br />

SOC<br />

Open circuit voltage Internal Resistance<br />

Fig. 9 – Battery internal parameters.<br />

Chart in Fig. 8 show the current intensity and voltage evolution in time<br />

and Fig. 9 show the battery parameters, Open Voltage E oc and internal<br />

resistance R int function of the battery state SOC.<br />

Another simulation done was with a simple cooling of the battery, and<br />

with a variable load resistor which changes the current drawn over time.<br />

Here we used a convection model to remove the heat from the battery and<br />

an ambient temperature of 20 o C.<br />

In Fig. 12 can be seen that the temperature and the current intensity are<br />

connected but there is a slight shift between the current maximum and the<br />

temperature maximum, this can be explained if we look at Fig. 11 and Fig. 9. In<br />

Fig. 11 can be observed that the maximum temperature is near a SOC of 0 and<br />

from Fig. 9ig. 9 we can see that at SOC near 0 the internal resistance rises so<br />

more heat will be generated.

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