One ideal core flux-change source feeds both windings. Exact arithmetic here means exact results for the stated model inputs; measured inputs still carry uncertainty and significant-figure limits.

highlighted = computed this step

Both windings cite one flux-change source

The flux change and interval are shared. Each winding multiplies that rate by its own turns.

V=NΔΦΔtV=N{\Delta\Phi\over\Delta t}
Shared flux setupBoth voltages cite the same flux-change source.Np 6Ns 3dPhi 1 Wbdt 1 sVp 6 VVs 3 Vmode aiding

Each winding voltage follows its own turns

The flux-rate row stays fixed while the turn counts change together.

NpNsVpVs212 V1 V424 V2 V636 V3 V\begin{array}{c|c|c|c}N_p&N_s&V_p&V_s\\2&1&2\ \text{V}&1\ \text{V}\\4&2&4\ \text{V}&2\ \text{V}\\6&3&6\ \text{V}&3\ \text{V}\\\end{array}

One flux change sets both winding voltages

The checked row has one shared flux source, one interval, and two winding turn counts.

V=NΔΦΔt66 V33 VV=N{\Delta\Phi\over\Delta t}\quad6\rightarrow6\ \text{V}\quad3\rightarrow3\ \text{V}
Shared flux ledgerBoth voltages cite the same flux-change source.Np 6Ns 3dPhi 1 Wbdt 1 sVp 6 VVs 3 Vmode aiding