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Capacitor notes and lesson for A Level physics (free PDF download)

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Capacitor notes and lesson for A Level physics (free PDF download)

This physics grades 11-12 lesson on capacitor notes gives the key ideas first, then worked examples and diagrams. After that, practise with the worksheet on capacitor and check yourself with the quiz.

Quick answer: A capacitor stores charge on two plates, and its capacitance is C = Q / V in farads. The stored energy is E = ½CV². Capacitors in parallel add, while series capacitors combine as reciprocals. Through a resistor the voltage changes exponentially with time constant τ = RC.

Level: Physics grades 11-12 (A Level · IB · Class 11-12) · Curriculum: A Level 3.7.4

Capacitor notes: the key ideas

What is a capacitor and what does capacitance mean?

A capacitor stores energy by keeping equal and opposite charges on two conducting plates separated by an insulator. The camera flash in a phone, the timer in a pedestrian crossing and the smoothing circuit in a charger all rely on this.

Definition

Capacitance is the charge stored per unit potential difference: C = Q / V. It is measured in farads (F); 1 F = 1 C/V. Most real capacitors are in microfarads (µF), nanofarads (nF) or picofarads (pF).

Here Q is the magnitude of the charge on one plate, not the total charge on the capacitor, which is always zero. A capacitor of larger capacitance stores more charge at the same voltage.

Formula

Q = CV

Q = charge on one plate (C), C = capacitance (F), V = potential difference across the capacitor (V). Unit prefixes: 1 µF = 10⁻⁶ F, 1 nF = 10⁻⁹ F, 1 pF = 10⁻¹² F.

How much energy does a capacitor store?

As charge builds up, each extra bit of charge must be pushed against a rising voltage. The graph of Q against V is a straight line, and the work done is the area under it.

Straight-line graph of charge against voltage for a 470 microfarad capacitor reaching 5.64 millicoulombs at 12 volts, with the triangle under the line shaded0481204812p.d. V (V)charge Q (mC)area = ½QVgradient = C
Q against V for a 470 µF capacitor. The gradient is C and the shaded area is the energy stored.
Key law

Energy stored: E = ½QV = ½CV² = Q² / 2C, with E in joules, Q in coulombs, C in farads and V in volts.

Worked example

A 470 µF capacitor is charged to 12 V. Calculate the charge and the stored energy.

Q = CV = 470 × 10⁻⁶ × 12 = 5.64 mC. E = ½CV² = 0.5 × 470 × 10⁻⁶ × 12² = 34 mJ.

How do capacitors combine in series and in parallel?

ArrangementTotal capacitanceWhat stays equal
ParallelC = C₁ + C₂ + …the voltage across each
Series1/C = 1/C₁ + 1/C₂ + …the charge on each

The rules for capacitors are the reverse of those for resistors: parallel capacitors add, and series capacitors combine through reciprocals. The total in series is always smaller than the smallest single capacitor.

Worked example

A 4.7 µF and a 10 µF capacitor are connected, first in series and then in parallel. Find each total.

Series: 1/C = 1/4.7 + 1/10 = 0.3128, so C = 3.2 µF. Parallel: C = 4.7 + 10 = 14.7 µF.

Common mistake

Do not copy the resistor rules. If you add series capacitances directly, the total comes out too large, because a series chain behaves like a single capacitor with a wider gap.

How does a capacitor charge and discharge through a resistor?

A resistor limits the current that flows to or from the capacitor, so the voltage changes gradually. The rate is set by the time constant.

Two circuits: a battery, resistor and capacitor in series for charging, and the same resistor and capacitor without the battery for dischargingRICchargingRICdischarging
Charging (left): the battery pushes charge through R onto the plates. Discharging (right): the stored charge flows back through R.
Formula

τ = RC

τ = time constant (s), R = resistance (Ω), C = capacitance (F). Discharging: V = V₀e−t/τ. Charging: V = V₀(1 − e−t/τ), where V₀ is the starting voltage on discharge or the supply voltage on charging.

TimeDischarging: V as fraction of V₀Charging: V as fraction of V₀
1τ0.370.63
2τ0.140.86
3τ0.050.95
5τ0.0070.993
Graph of the voltage across a discharging capacitor falling exponentially from 9.0 volts, with a marker at 3.3 volts after 22 seconds, one time constant02040600246810time t (s)p.d. across capacitor V (V)0.37 V₀ at t = τ = 22 s
Discharge of a capacitor through a resistor (V₀ = 9.0 V, τ = 22 s). The voltage falls to 37 % after one time constant.
Worked example

A 220 µF capacitor discharges from 9.0 V through 100 kΩ. Find V after 30 s and the time for V to fall to 1.0 V.

τ = RC = 100 × 10³ × 220 × 10⁻⁶ = 22 s. After 30 s, V = 9.0 e−30/22 = 2.3 V. For 1.0 V: t = τ ln(V₀/V) = 22 × ln 9.0 = 48 s.

Lina’s tip

Count in time constants: a discharging capacitor keeps 37 %, 14 % and 5 % of its voltage after one, two and three time constants. It is practically flat after about 5τ.

Key points to remember
  • C = Q / V; 1 farad = 1 coulomb per volt
  • Energy stored E = ½CV² = ½QV = Q² / 2C
  • Parallel: C = C₁ + C₂; series: 1/C = 1/C₁ + 1/C₂
  • Time constant τ = RC; discharging V = V₀e^(−t/τ)
  • After 1τ a capacitor has lost 63 % of its charge (discharging) or reached 63 % (charging)

Charge storage, energy and RC time constants: frequently asked questions

What does one farad mean?

One farad is one coulomb of charge stored per volt across the capacitor. It is a huge unit, so everyday capacitors have values between picofarads and a few thousand microfarads.

Why does the current fall as a capacitor charges?

The voltage across the capacitor rises and opposes the supply voltage, so the voltage across the resistor, and therefore the current, shrinks. The current becomes zero when the capacitor voltage equals the supply voltage.

What is the time constant of an RC circuit?

It is τ = RC, the time for a discharging capacitor to fall to 37 % of its starting voltage. It is also the time for a charging capacitor to reach 63 % of the supply voltage.

Why is the energy ½CV² and not CV²?

The voltage rises from zero as the charge is added, so on average only half of the final voltage acts on each bit of charge. The area under the Q–V graph is a triangle, which gives one half.

What happens to the energy of a discharging capacitor?

It is transferred to the resistor as thermal energy as the current flows. For a capacitor discharging completely, the total energy dissipated equals the initial stored energy ½CV².

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