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PhD Thesis - Cranfield University

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Chapter 3<br />

Battery<br />

Voc<br />

Ri<br />

Vb i<br />

Test circuit to measure Ri DC<br />

S2<br />

Ib i<br />

S1<br />

R1<br />

R2<br />

Vb 0 Vb 3<br />

Vb 1<br />

Vb 2<br />

71<br />

Ib 1<br />

S1=1<br />

Ib 2<br />

S1,S2=1<br />

S1,S2=0<br />

Voltage and current traces during an Ri measurement experiment<br />

Figure 3.6 Tests to measure the DC internal resistance of a battery.<br />

The exponential decay and rise of the voltage traces shown in the Figure 3.6 is due to the<br />

lead capacitance of the measuring instrumentation. This capacitance does not influence the<br />

DC resistance measurement, which is calculated based on voltage measurement points taken<br />

when the battery voltage trace is parallel to the horizontal axis.<br />

3.14 Determining Battery Operating Constraints<br />

Maximum Discharging Power<br />

The maximum discharging power of a battery system is limited by the maximum allowable<br />

discharging current, minimum terminal voltage and temperature. Theoretically, the<br />

maximum current that the battery can deliver occurs when the battery is at full charge and<br />

the internal resistance is at its minimum value. However, in practice, specification of the<br />

maximum discharging current (Ibattmax) is normally limited by mandatory safe operating<br />

conditions of the battery as well as the current handling capacity of the electrodes itself. The<br />

limitation in discharging power due to the current constraint can be expressed as,<br />

2<br />

dis max batt<br />

[ SoC ] batt<br />

[ SoC ]<br />

Pb = I max ( Voc ) − I max ( Ri )<br />

( 3-28)

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