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CR · Energy storage

Energy in Capacitors and Inductors

Capacitors and inductors do not merely impede current — they hold energy for a while. Learn how that stored amount depends on voltage or current, and why it grows as the square.

Energy grows as the square of voltage

Slide the voltage V across the capacitor and watch the stored energy. The curve is not a straight line — it keeps steepening. Set the voltage so the stored energy reaches the target of 18 mJ.

Voltage VV = 2.0 V
Stored energy
E = 2.0 mJ
E = ½CV² (C = 1 mF)
Far from target

Two ways to bank up work

A capacitor stores energy in the electric field between its plates. Raising the voltage means pushing charge in, and the charge already there pushes back on the next, so the work to add more keeps growing. An inductor stores energy in the magnetic field around its coil. Raising the current means working against the coil’s opposition (its induced voltage), which is stronger the larger the current. Both store only temporarily and give it back when needed.

Why the square appears

In a capacitor the charge is proportional to the voltage (Q = CV). While raising the voltage from 0 to V, the average voltage is half of V, and the work put in is average voltage times total charge: ½·V·(CV) = ½CV². The half comes from averaging a linear rise that starts at zero; the square comes from voltage and charge growing together in proportion. An inductor follows the same logic to give ½LI².

The square magnifies small differences

The square relation means doubling the voltage quadruples the energy; tripling it makes it nine times. So to greatly increase the energy in a capacitor, raising the voltage is far more effective than raising the capacitance — and conversely, even a small overvoltage can swell the stored energy dangerously. Because this energy pours out all at once on discharge, large capacitors call for care in handling.

ObserveEC = ½CV²
A capacitor goes as voltage squared.
ChooseV ×2 → E ?
Squared, so double means quadruple.
Fill inEL = ½L ?
An inductor goes as current squared.
On your ownV = ?
Solve the voltage from the target energy.

Back to the first screen

As you slid the voltage, the stored energy traced not a line but a curve that kept steepening, and it reached the target of 18 mJ at V = 6 V. For the same capacitance, a little more voltage raised the energy by that much squared. The capacitor’s ½CV² and the inductor’s ½LI² are the same shape, and the energy the two elements traded in transients and resonance was exactly this stored amount.

A capacitor’s stored energy is ½CV², proportional to voltage squared, and an inductor’s stored energy is ½LI², proportional to current squared. Because it is a square, doubling the value quadruples the energy. Both store energy temporarily in a field, and the voltage needed for a target energy is V = √(2E/C).