A double-current-quadruples-energy scan holds the inductance fixed and varies the current across three rows, checking that stored energy E = L * I^2 / 2 rises with the square of current row by row. The arithmetic is exact only for the stated inductances, currents, stored energies, and rows in the ideal lossless inductor model. Real inductors add winding resistance, core saturation, core loss, switch loss, current-sense/probe calibration limits, finite precision, and measurement uncertainty.

Changing only current exposes the square in the energy law. Exact arithmetic here means exact results for the stated model inputs; measured inputs still carry uncertainty and significant-figure limits.

highlighted = computed this step

Current is the squared variable

The inductance stays at 2 H. Changing current changes stored energy by the square.

E∝I2when L is fixedE\propto I^{2}\quad\text{when }L\text{ is fixed}
Current-square setupThe current value is squared before energy is accepted.L 2 HI 3 AE 9 JI0 0 AE0 0 JdE 9 J

Energy grows by the square of current

The rows show why a doubled current stores four times as much energy in the same inductor.

LIE2 H1 A1 J2 H3 A9 J2 H6 A36 J\begin{array}{c|c|c}L&I&E\\2\ \text{H}&1\ \text{A}&1\ \text{J}\\2\ \text{H}&3\ \text{A}&9\ \text{J}\\2\ \text{H}&6\ \text{A}&36\ \text{J}\\\end{array}

Doubling current quadruples the stored energy

The inductor is unchanged. The current is squared before the energy is computed.

3 A→9 J;6 A→36 J3\ \text{A}\rightarrow9\ \text{J}\quad;\quad6\ \text{A}\rightarrow36\ \text{J}
Current-squared energy contrastThe higher current case stores four times the energy.L 2 HI 3 AE 9 JI0 0 AE0 0 JdE 9 JL 2 HI 6 AE 36 JI0 0 AE0 0 JdE 36 J