A constant inductor voltage over a finite interval fixes the current ramp. Exact arithmetic here means exact results for the stated model inputs; measured inputs still carry uncertainty and significant-figure limits.

highlighted = computed this step

The ramp starts with one fixed inductance

The inductor is 2 H. A constant voltage over a declared interval gives a finite current change.

V=LΔIΔtΔI=VΔtLV=L{\Delta I\over \Delta t}\quad\Rightarrow\quad \Delta I={V\Delta t\over L}
Inductor ramp setupThe ramp check binds voltage, time, inductance, and current change.L 2 HV 6 Vdt 1 sIi 0 AdI 3 AIf 3 A

More voltage gives a larger current change

The inductance and interval stay fixed, so the current-change rows scale with applied voltage.

LVΔtΔI2 H2 V1 s1 A2 H4 V1 s2 A2 H6 V1 s3 A\begin{array}{c|c|c|c}L&V&\Delta t&\Delta I\\2\ \text{H}&2\ \text{V}&1\ \text{s}&1\ \text{A}\\2\ \text{H}&4\ \text{V}&1\ \text{s}&2\ \text{A}\\2\ \text{H}&6\ \text{V}&1\ \text{s}&3\ \text{A}\\\end{array}

Voltage times time sets the inductor current change

The interval is a declared constant-voltage training interval, so the checked ramp is finite and exact.

ΔI=VΔtL=6 V1 s/2 H=3 A\Delta I={V\Delta t\over L}=6\ \text{V}\cdot1\ \text{s}/2\ \text{H}=3\ \text{A}
Inductor current rampThe current-change label is generated from V, t, and L.L 2 HV 6 Vdt 1 sIi 0 AdI 3 AIf 3 A