A switch-on interval raises inductor current by a checked amount. Exact arithmetic here means exact results for the stated model inputs; measured inputs still carry uncertainty and significant-figure limits.

highlighted = computed this step

On-time uses the positive inductor voltage

The inductance and interval are fixed. The positive switch-on voltage sets the upward ripple slope.

ΔIon=VonΔtL\Delta I_{\text{on}}={V_{\text{on}}\Delta t\over L}
Switch-on interval setupThe on interval raises the inductor current.L 3 HV 9 Vdt 1 sIi 0 AdI 3 AIf 3 A

Larger on voltage builds more ripple in the same time

Each row uses the same inductor and the same interval, so the current step follows voltage.

LVonΔtΔI3 H3 V1 s1 A3 H6 V1 s2 A3 H9 V1 s3 A\begin{array}{c|c|c|c}L&V_{\text{on}}&\Delta t&\Delta I\\3\ \text{H}&3\ \text{V}&1\ \text{s}&1\ \text{A}\\3\ \text{H}&6\ \text{V}&1\ \text{s}&2\ \text{A}\\3\ \text{H}&9\ \text{V}&1\ \text{s}&3\ \text{A}\\\end{array}

The on interval builds a finite ripple current

The on-state inductor voltage is declared, then the current change is computed from that exact interval.

ΔIon=9 V1 s/3 H=3 A\Delta I_{\text{on}}=9\ \text{V}\cdot1\ \text{s}/3\ \text{H}=3\ \text{A}
Switch-on ripple intervalThe on interval raises the inductor current.L 3 HV 9 Vdt 1 sIi 0 AdI 3 AIf 3 A