Section 1 of 7Reading an I–V graph
What is plotted
- What is plotted An I–V graph shows how the current I through a component changes as the potential difference V across it is varied.
- Conventionally current is on the y-axis and potential difference on the x-axis.
Link to resistance
- Link to resistance Resistance is found from R = V ÷ I, so it can be worked out from any single point on the graph.
- The resistance is not simply the gradient unless the graph is a straight line through the origin.
Reversing the cell
- Reversing the cell Swapping the connections to the power supply reverses the current, so the graph continues into the negative quadrants.
- For an ohmic conductor and a filament lamp the negative part is a mirror image of the positive part.
Section 2 of 7Ohmic conductors
Straight line through the origin
Ohm's law
- Ohm's law At constant temperature the current through an ohmic conductor is directly proportional to the potential difference across it.
Constant resistance
- Constant resistance Doubling V doubles I,
- so the ratio V ÷ I never changes: V = I × R.What the symbols mean: V = potential difference (V) · I = current (A) · R = resistance (Ω)
- so the ratio V ÷ I never changes: V = I × R.
Examples
- Examples Fixed resistors and metal wires kept at a constant temperature.
Steepness
- Steepness A steeper line means a larger current for the same p.d., so a smaller resistance.
Section 3 of 7Why a filament lamp curves
1Current flows
- Current flows Electrons collide with the metal ions of the filament, transferring energy to them.
2Filament heats up
- Filament heats up The ions vibrate with larger amplitude as the temperature rises.
3More collisions
- More collisions Electrons are obstructed more often, so it is harder for charge to flow.
4Resistance increases
- Resistance increases Current rises by less and less for each equal step in p.d., so the graph flattens into a curve.
Section 4 of 7Comparing components
| Component | Shape of I–V graph | Resistance behaviour |
|---|---|---|
| Fixed resistor | Straight line through the origin | Constant |
| Filament lamp | S-shaped curve, steeper near the origin | Increases as the filament gets hotter |
| Diode | Almost no current in reverse; current rises sharply once forward p.d. passes about 0.6 V | Very high in reverse, low in the forward direction |
| Thermistor (NTC) | Curve getting steeper as it warms | Decreases as temperature rises |
Section 5 of 7Diode in detail
1
A diode only allows current to pass in one direction, the direction of the arrowhead in its symbol.
2
In the forward direction the current is negligible until the p.d. reaches a threshold of a few tenths of a volt.
3
Above the threshold the current increases rapidly, so the resistance drops.
4
In the reverse direction the resistance is so high that the current is effectively zero.
Section 6 of 7Key terms
| Term | Meaning |
|---|---|
| Ohmic conductor | A conductor whose current is directly proportional to p.d. at constant temperature. |
| Non-ohmic conductor | A component whose resistance changes as the current or conditions change, giving a curved I–V graph. |
| Potential difference | The energy transferred per unit charge between two points, measured in volts. |
| Resistance | A measure of how much a component opposes current, found using R = V ÷ I and measured in ohms (Ω). |
| Diode | A component that lets current flow in one direction only. |
Section 7 of 7Exam technique
1
Saying the resistance of a lamp is the gradient of its curve — use R = V ÷ I at a chosen point instead.
2
Claiming the filament lamp's resistance increases because the current is bigger without mentioning the rise in temperature.
3
Thinking a steeper I–V line means a larger resistance — it means a smaller one, because more current flows per volt.
4
Forgetting that a graph with the axes swapped (V against I) has its steep and shallow meanings reversed.