3.6 Thevenin's theorem 51
and B at either end of the resistor, r. To calculate E0 we first remove the resistor
r in the circuit of Fig. 3.18 to give the circuit of Fig. 3.20.
To calculate the potential difference between A and B we need to determine
(~20V
I 20s
I oA
lOV
~
lOfl
oB
Figure 3.20
the current I. Applying KVL to the closed path and taking the clockwise
direction to be positive
20- 51- 101- 10 = 0
151 = 10
I = 0.67 A
The potential drop between A and B is then given by
VAB -- IR 2 -Jr V 2 .~- 0.67 • 10 + 10 = 16.7 V
Since this turns out to be positive, then the potential of terminal A is higher
than that of terminal B and the current IL flOWS from A to B.
In accordance with Thevenin's theorem, VAB = E0.
To calculate R0 we remove the resistor r in Fig. 3.18 and replace the batteries
20~
-4 ] oA
.•5•
[~10~
oB
Figure 3.21
by short circuits to give the diagram of Fig. 3.21. R0 is the resistance between A
and B and is given by
RAB- R3 + R1R2//(R1 + R2)
= 20 + 50/15
= 23.33 11
Now from the Thevenin equivalent circuit of Fig. 3.19, putting in the values for
E0 and R0,