66Electric
Vehicle Technology Explained, Second Edition
3.12.2 Battery Equivalent CircuitThe first task in simulating the performance of a battery is to construct an equivalent circuit. This is
a circuit made up of elements, and each element has precisely predictable behaviour.
We introduced such an equivalent circuit at the beginning of this chapter. Figure 3.1 is a very simple (but still highly useful) equivalent circuit fora battery. A limitation of this type of circuit is that it does not explain the dynamic behaviour of the battery at all. For example, if a load is connected to the battery the voltage will immediately change to anew (lower) value. In fact this is not true rather the voltage takes time to settle down to anew value.
Figure 3.17 shows a somewhat more refined equivalent circuit that simulates or models these dynamic effects quite well. We could carry on refining our circuit more and more to give an ever-closer prediction of performance. These issues are discussed in the literature,
for
example by Johnson, Zolot and Pesaran (The purpose of our battery simulations is to be able to predict the performance of EVs,
in terms of range,
acceleration, speed, and soon a topic covered in reasonable depth in Chapter 8. In these simulations the speed of the vehicles changes fairly slowly, and the dynamic behaviour of the battery makes a difference that is small compared with the other approximations we have to make along the way. Therefore, in this introduction to battery simulation we will use the basic equivalent circuit of Figure Although the equivalent circuit of Figure 3.1
is simple, we do need to understand that the values of the circuit parameters (
E and
R) are not constant. The open-circuit voltage of the battery
E is the most important to establish first. This changes with the state of charge of the battery.
In the case of the sealed lead acid battery we have already seen that the open-circuit voltage
E is approximately proportional to the
state of charge of the battery, as in Figure This shows the voltage of one cell of a battery. If we propose a battery variable
DoD ,
meaning the depth of discharge of a battery, which is 0 when fully charged and 1.0
when empty, then the simple formula for the open-circuit voltage is
E =
n × [2
.15 −
DoD ×
(2
.15 − 2
.00
)]
(3.16)
E
R
2
I
V
R
1
C
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