Ohm’s law states that the current through a conductor is directly proportional to the potential difference across it, provided the temperature remains constant.
The formula
V = I R
where V is potential difference in volts (V), I is current in amperes (A), and R is resistance in ohms.
This can be rearranged to: I = V / R or R = V / I
Ohmic and non-ohmic conductors
A component that obeys Ohm’s law is called an ohmic conductor. Its V-I graph is a straight line through the origin. The gradient of this line equals the resistance (which stays constant).
Examples of ohmic conductors: a metal wire at constant temperature, a resistor.
Non-ohmic components have V-I graphs that are not straight lines:
- Filament lamp: resistance increases as temperature rises, so the graph curves.
- Diode: current flows in one direction only; the graph shows a sharp rise after the threshold voltage and is flat (zero current) in the reverse direction.
- Thermistor: resistance decreases as temperature increases.
Experimental verification
To verify Ohm’s law for a resistor:
- Set up a circuit with a power supply, variable resistor, ammeter (in series), and voltmeter (in parallel with the test resistor).
- Adjust the variable resistor to change the current.
- Record the ammeter and voltmeter readings for each setting.
- Plot V (y-axis) against I (x-axis).
- If the graph is a straight line through the origin, the resistor obeys Ohm’s law. The gradient equals the resistance.
Need help understanding this?
A 0625 specialist can explain this concept using the student's own questions and show how it appears in exam papers.