EG1216 · Physics 2 — Electricity & Magnetism
Theme 2 · Electric potential & capacitance

Energy stored in a capacitor

Charging a capacitor stores energy in it — energy a camera flash or a defibrillator dumps out in a fraction of a second.

Source: Serway & Jewett, Physics for Scientists and Engineers, 7th ed., §26.4.

Before you start

What you need first

  • Topic 12 — \(C = Q/V\) and \(Q = CV\).
  • Topic 9 — moving charge through a voltage costs energy.
  • Energy in joules; area of a triangle.

What you'll be able to do

  • Use \(U = \tfrac12 CV^2\) for the stored energy.
  • Switch to the forms \(U = \tfrac12 QV\) and \(U = \dfrac{Q^2}{2C}\).
  • See why the energy is the area under the \(Q\)–\(V\) line.

The result

Energy stored

Charging a capacitor means pushing charge onto the plates against a voltage that keeps rising. The total energy stored works out to:

$$ U = \tfrac12 CV^2 $$
where:
SymbolMeaningSI unit
Uenergy stored in the capacitorJ
CcapacitanceF
Vvoltage across itV
Three forms, one energy. Using \(Q = CV\) you can also write \(U = \tfrac12 QV = \dfrac{Q^2}{2C}\). Pick whichever matches what you are given.

Why the factor of ½?

As you add charge, the voltage grows in proportion: \(Q = CV\) is a straight line. The energy is the area under that line — a triangle, whose area is \(\tfrac12 \times \text{base} \times \text{height} = \tfrac12 QV\).

The last bit of charge costs the full voltage, but the first bit cost almost nothing — so you pay the average, half the final voltage. That is where the \(\tfrac12\) comes from.
V Q ½QV V Q = CV
\(Q\) rises in step with \(V\); the shaded triangle (area \(\tfrac12 QV\)) is the stored energy.
📐 Worked example 1

Energy from C and V

A \(C = 5.0\ \mu\text{F}\) capacitor is charged to \(V = 12\) V. Find the energy stored.

1Use \(U = \tfrac12 CV^2\) (square the voltage: \(12^2 = 144\)):
$$ U = \tfrac12 (5.0\times10^{-6})(12)^2 = \tfrac12 (5.0\times10^{-6})(144) $$
2Work it out:
$$ U \approx 3.6\times10^{-4}\ \text{J} $$
📐 Worked example 2

Energy from Q and C

A \(C = 10\ \mu\text{F}\) capacitor holds \(Q = 50\ \mu\text{C}\). Find the energy stored.

1Here \(Q\) and \(C\) are given, so use \(U = Q^2/2C\):
$$ U = \frac{(50\times10^{-6})^2}{2(10\times10^{-6})} $$
2Work it out:
$$ U \approx 1.25\times10^{-4}\ \text{J} $$
Same energy whichever form you use — choose the one that fits the given quantities.

✏️ Try it yourself

A camera-flash capacitor of \(C = 200\ \mu\text{F}\) is charged to \(V = 300\) V.

(a) Find the energy it stores.
(b) If it were charged to twice the voltage, how would the energy change?

(a) Step 1. \(U = \tfrac12 CV^2 = \tfrac12 (200\times10^{-6})(300)^2.\) Step 2. \(U = \tfrac12 (200\times10^{-6})(90000) \approx 9.0\ \text{J}\) (enough for a bright flash). (b) Energy goes as \(V^2\), so doubling the voltage gives four times the energy — about \(36\) J.

Common mistakes

MistakeFix
Forgetting to square \(V\).\(U = \tfrac12 CV^2\) — the voltage is squared.
Dropping the \(\tfrac12\).The energy is the triangle area, so the factor of \(\tfrac12\) is always there.
Mixing the three forms.\(\tfrac12 CV^2\), \(\tfrac12 QV\), \(Q^2/2C\) are equal — don't combine pieces of different ones.
Leaving µF or µC unconverted.Convert to F and C before computing.

Recap — the whole topic on one screen

IdeaWhat you own now
Stored energy\(U = \tfrac12 CV^2 = \tfrac12 QV = \dfrac{Q^2}{2C}\).
The ½Energy is the area under the \(Q\)–\(V\) line (a triangle).
ScalingEnergy goes as \(V^2\): double the voltage → four times the energy.

Next topic

Dielectrics

Slide an insulator into the gap and the capacitance jumps. Next we see how a dielectric boosts \(C\) — and lets a capacitor hold more charge and energy.

→ Topic 15 · Dielectrics