Revision Notes
AQA A-Level Physics: Electricity (7408) – Revision Notes
Condensed AQA A-Level Physics 7408 Electricity notes: key equations, I-V graphs, resistivity, circuit rules, potential dividers and a quick self-test.
- Subject
- Physics
- Level
- A LEVELS
- Topic
- Electricity
- Author
- Marlbridge Academic Team
- Updated
Aligned to AQA A Level Physics (7408), For first teaching 2015. Official specification .
Syllabus page (what it covers and how it is assessed): AQA A Level Physics.
Syllabus points this page covers
7408
- 3.5.1 Current electricity
- 5 Electricity (whole topic)
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Condensed for the final weeks. For full explanations and worked examples, use the Electricity study guide.
These notes cover section 3.5 Electricity (3.5.1.1 to 3.5.1.6) of the AQA AS and A-level Physics specification (7407/7408, version 1.4, AS and A-level exams June 2016 onwards). It is AS and A-level content: at A-level it is assessed in Paper 1 and assumed in Paper 2. It is not one of the options (sections 3.9 to 3.13), one of which you study for Paper 3 Section B. Test yourself afterwards with the practice questions, the course hub, the printable checklist and the free diagnostics.
Equations
| Equation | Meaning | Units |
|---|---|---|
| I = ΔQ/Δt | current = rate of flow of charge | A = C s⁻¹ |
| V = W/Q | pd = work done per unit charge | V = J C⁻¹ |
| R = V/I | definition of resistance | Ω = V A⁻¹ |
| ρ = RA/L | resistivity | Ω m |
| R_T = R₁ + R₂ + … | resistors in series | Ω |
| 1/R_T = 1/R₁ + 1/R₂ + … | resistors in parallel | Ω |
| E = IVt | energy transferred | J |
| P = IV = I²R = V²/R | power | W |
| ε = E/Q | emf = energy transferred per unit charge by the source | V |
| ε = I(R + r) | emf with internal resistance | V |
3.5.1.1 Definitions
- Current: rate of flow of charge.
- Potential difference: work done per unit charge.
- Resistance: R = V/I, valid at any point on any I–V graph.
- Emf: energy transferred to electrical form per unit charge by the source.
3.5.1.2 I–V characteristics
| Component | Shape (I on vertical axis) | Reason |
|---|---|---|
| Ohmic conductor | Straight line through origin | R constant at constant temperature |
| Filament lamp | Gradient falls as V rises; symmetrical | Hotter filament → ions vibrate more → R rises |
| Semiconductor diode | ~0 current below a threshold pd, then steep rise; ~0 in reverse | Conducts in one direction only |
Ohm’s law: I ∝ V under constant physical conditions. It is a special case, not a definition of resistance.
Ideal meters (unless told otherwise): ammeter zero resistance, voltmeter infinite resistance.
With V on the horizontal axis the lamp curve flattens; with I on the horizontal axis it steepens. Either way R rises. Read the axes first.
3.5.1.3 Resistivity and temperature
Method in steps: ρ from a wire
- Convert the diameter to metres.
- A = πd²/4.
- ρ = RA/L, or ρ = gradient × A from an R against L graph.
Ratio reminder: R ∝ L/d². Double L → R doubles. Double d → R falls to a quarter.
- Metals: R increases with temperature.
- ntc thermistors (the only type assessed): R decreases as temperature increases. Used as temperature sensors; the R–T graph is a falling curve.
- Superconductor: zero resistivity at and below a critical temperature, which depends on the material. Uses: strong magnetic fields; less energy loss in power transmission. Critical field is not assessed.
Required practical 5: micrometer for d (several readings, several orientations); ammeter and voltmeter for R at several lengths; plot R against L; gradient = ρ/A. Small currents to avoid heating.
3.5.1.4 Circuit rules
| Series | Parallel | |
|---|---|---|
| Current | same everywhere | splits; branch currents add |
| Pd | shared; pds add | same across each branch |
| Total R | larger than the largest | smaller than the smallest |
- Conservation of charge → current into a junction = current out.
- Conservation of energy → round a loop, sum of emfs = sum of pds.
- Cells in series: emfs add (watch direction), internal resistances add.
- n identical cells in parallel: emf of one cell, internal resistance r/n.
Method in steps: series–parallel network
- Replace each parallel group with its single equivalent resistance.
- Add series resistances to get R_T.
- I = V/R_T from the supply.
- Work back out: pd across each part, then branch currents.
- Check that branch currents add to the total and pds round each loop add to the emf.
3.5.1.5 Potential divider
V_out = V_in × R₂/(R₁ + R₂), with V_out across R₂.
- Fixed resistors → constant output. Variable resistor → variable output.
- Thermistor: hotter → R falls → its share of the pd falls.
- LDR: brighter → R falls → its share of the pd falls.
- To make V_out rise with temperature, take it across the fixed resistor (in series with the thermistor). To make it rise in the dark, take it across the LDR.
- A load across the output is in parallel with R₂ and lowers V_out.
- The potentiometer as a measuring instrument is not required.
3.5.1.6 Emf and internal resistance
- ε = I(R + r) = V + Ir
- Terminal pd V = IR = ε − Ir. It falls as current rises.
- Lost volts = Ir.
- Open circuit (I = 0): terminal pd = ε.
Required practical 6: vary an external resistor, record terminal pd V and current I. Plot V against I: gradient = −r, y-intercept = ε.
Small worked reminders
Resistance from resistivity. A wire 2.0 m long has cross-sectional area 1.0 × 10⁻⁷ m² and ρ = 1.7 × 10⁻⁸ Ω m.
R = ρL/A = 1.7 × 10⁻⁸ × 2.0 / 1.0 × 10⁻⁷ = 0.34 Ω
Emf from two readings. Terminal pd is 5.6 V at 0.40 A and 4.8 V at 1.20 A.
r = ΔV/ΔI = (5.6 − 4.8) / (1.20 − 0.40) = 1.0 Ω
ε = V + Ir = 5.6 + 0.40 × 1.0 = 6.0 V
LDR divider. A 5.0 V supply feeds a 4.0 kΩ resistor in series with an LDR; V_out is across the LDR. In light the LDR is 1.0 kΩ; in the dark it is 16 kΩ.
light: V_out = 5.0 × 1.0 / 5.0 = 1.0 V
dark: V_out = 5.0 × 16 / 20 = 4.0 V
Opposing cells. A 6.0 V cell and a 1.5 V cell in series but facing opposite ways give a net emf of 6.0 − 1.5 = 4.5 V.
Must-know distinctions
- Emf vs pd: emf is energy given to each coulomb by the source; pd is energy transferred from each coulomb by a component.
- Resistance vs resistivity: R depends on shape; ρ is a property of the material (at a given temperature).
- R = V/I vs gradient: on a curved graph these differ. Resistance is always V/I.
- Metal vs ntc thermistor: opposite temperature behaviour.
- Cells in series vs identical cells in parallel: series raises emf; parallel keeps emf and cuts internal resistance.
Quick self-test
- A charge of 4.8 C passes a point in 3.0 s. Find the current.
- 7.5 J of work is done moving 2.5 C between two points. Find the pd.
- Find the total resistance of three 6.0 Ω resistors in parallel.
- A 2.0 Ω and a 3.0 Ω resistor are in series across a 10 V supply of negligible internal resistance. Find the current and the power in the 3.0 Ω resistor.
- A wire has resistance 2.0 Ω. Find the resistance of a wire of the same material with twice the length and twice the diameter.
- A source of emf 6.0 V and internal resistance 1.0 Ω is connected to a 5.0 Ω resistor. Find the current and the terminal pd.
- A 12 V supply is connected across a 3.0 kΩ and a 1.0 kΩ resistor in series. Find the pd across the 1.0 kΩ resistor.
- State what happens to the resistance of an ntc thermistor when it is heated.
- State the resistance of an ideal voltmeter.
- A 60 W lamp runs on 230 V for 2.0 hours. Find the current and the energy transferred.
- State the resistivity of a superconductor below its critical temperature.
- State what the gradient of a graph of terminal pd against current gives.
Answers
- I = 4.8/3.0 = 1.6 A
- V = 7.5/2.5 = 3.0 V
- 1/R = 3/6.0, so R = 2.0 Ω
- I = 10/5.0 = 2.0 A; P = I²R = 2.0² × 3.0 = 12 W
- R ∝ L/d²: 2.0 × 2/2² = 1.0 Ω
- I = 6.0/(5.0 + 1.0) = 1.0 A; V = IR = 5.0 V
- V = 12 × 1.0/4.0 = 3.0 V
- It decreases.
- Infinite.
- I = 60/230 = 0.26 A; E = Pt = 60 × 7200 = 4.3 × 10⁵ J
- Zero.
- −r (minus the internal resistance).
Where marks are usually lost
- Writing “pd is the energy per charge” without “work done” or “transferred”, or confusing it with emf.
- Using the gradient of a curved I–V graph as the resistance.
- Forgetting to convert mm to m, or squaring the diameter but forgetting the ÷4 in A = πd²/4.
- Leaving 1/R_T as the answer instead of taking the reciprocal.
- Explaining the filament lamp graph without the chain: current → temperature → ion vibration → resistance.
- Describing the thermistor in the wrong direction (only ntc thermistors are assessed).
- Using the supply emf as the terminal pd when internal resistance is not negligible.
- Giving the superconductor “very low” resistance rather than zero resistivity at and below the critical temperature.
- Forgetting that a load across a potential divider output reduces V_out.
Official syllabus
AQA AS and A-level Physics specification (7407/7408), version 1.4, July 2026, for AS and A-level exams June 2016 onwards, published by AQA. Section 3.5 Electricity.
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