The inductor ramp quotient is scanned with three exact rows. 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 change is voltage time divided by inductance

Each row is a full checked inductor ramp. The numerator is voltage times interval; inductance is the denominator.

ΔI=VΔtL\Delta I={V\Delta t\over L}
Ramp relation setupThe ramp check binds V, time, L, and current change.L 4 HV 8 Vdt 3 sdI 6 AL 4 HV 8 Vdt 3 sIi 0 AdI 6 AIf 6 A

Three ramp rows expose every part of the quotient

The rows change voltage, interval, and inductance, but every current change is computed by the same checked relation.

LVΔtVΔtΔI2 H6 V1 s6 Vs3 A3 H6 V2 s12 Vs4 A4 H8 V3 s24 Vs6 A\begin{array}{c|c|c|c|c}L&V&\Delta t&V\Delta t&\Delta I\\2\ \text{H}&6\ \text{V}&1\ \text{s}&6\ \text{V}\cdot\text{s}&3\ \text{A}\\3\ \text{H}&6\ \text{V}&2\ \text{s}&12\ \text{V}\cdot\text{s}&4\ \text{A}\\4\ \text{H}&8\ \text{V}&3\ \text{s}&24\ \text{V}\cdot\text{s}&6\ \text{A}\\\end{array}

The displayed current change comes from the checked ramp

The final row is not hand-labeled: the same source object displays the voltage, time, inductance, current change, and final current.

ΔI=8 V3 s/4 H=6 A\Delta I=8\ \text{V}\cdot3\ \text{s}/4\ \text{H}=6\ \text{A}
Ramp relation accepted rowThe current-change label is generated from the relation.L 4 HV 8 Vdt 3 sdI 6 AIf 6 AL 4 HV 8 Vdt 3 sIi 0 AdI 6 AIf 6 A