Energy stored in a capacitor

Physics A2 · Capacitance. The idea in plain words, the rules to remember, the mistake to avoid and a worked example, written and checked by Mega Lecture.

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The idea

Work must be done to charge a capacitor, because each new bit of charge is pushed onto a plate that already repels it. This work is stored as electric potential energy.

The p.d. is proportional to the charge (V = Q/C), so a graph of V against Q is a straight line through the origin. The energy stored is the area under this graph, which is a triangle: half base times height.

The factor of a half is there because the p.d. rises from zero to V during charging. The average p.d. is ½V, so the work done is Q × ½V, not QV.

Rules to remember

Common mistake

When the p.d. falls from V1 to V2, students use ½C(V1 − V2)2. Square each p.d. first and then subtract. Also change μF to F before calculating.

Worked example

A 470 μF capacitor is charged to a p.d. of 9.0 V. How much energy does it store?

  1. Change the unit: C = 470 × 10−6 F.
  2. W = ½CV2 = ½ × 470 × 10−6 × 9.02.
  3. W = ½ × 470 × 10−6 × 81 = 0.019 J.

Answer: 0.019 J (19 mJ)

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