Grade 11 Electric circuits R Toerien Page 26
Experimental determination of the internal resistance and emf of a battery
Different experiments can be done to determine the emf and internal resistance of a battery. Below are
three different experimental setups, using similar equipment, but drawing different graphs to determine the
internal resistance and the emf of a battery.
Experiment 1: Finding the internal resistance and emf of a battery
Learners set up a circuit according to the circuit diagram below to determine the internal resistance and emf
of a battery. The rheostat (variable resistor) was adjusted to ensure different readings for the total current in
the circuit. The potential difference was recorded for each current reading as shown in the table below.
Rheostat
adjustment
Current (A) Potential
difference (V)
1 0,3 2,80
2 0,4 2,68
3 0,5 2,60
4 0,6 2,50
5 0,7 2,42
6 0,8 2,30
In this experiment, the current was controlled (independent variable) by manipulating the rheostat. The
resistance of the rheostat started high so that the current is low. The resistance of the rheostat is then
decreased so that the current will increase by 0,1 A each time. In between each reading, the switch is
opened to prevent the circuit from heating up. This is done because temperature affects resistance. As the
total resistance decreased (RT↓) the total current increased (IT↑). The voltmeter reading decreased each
time. The voltmeter measured the potential difference of the external circuit (Vext) which is the dependent
variable. A graph of V versus I is drawn as shown below.
The y-intercept and gradient are used to determine the emf and internal resistance.
3,1
3,0
2,9
2,8
2,7
2,6
2,5
2,4
2,3
0,1 0,2 0,3 0,4 0,5 0,6 0,7 0,8 0,9 1,0
Current strength I (A)
Potential difference V (V)
Graph of potential difference (V) versus current strength (I)
Gradient =
∆V
∆I
=
2,3 – 2,8
0,8 – 0,3
=
– 0,5 V
0,5 A
= –1 Ω
gradient (m) = –r
∴ internal resistance (r) = 1 Ω
y-intercept = 3,1 V
y-intercept (c) = emf
∴ emf = 3,1 V
A
V
r