BULETINUL INSTITUTULUI POLITEHNIC DIN IAŞI
buletinul institutului politehnic din iaşi - Universitatea Tehnică ...
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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.