The Ideal Transformer and the Turns Ratio
What is conserved as you turn the ratio?
A single flux threads both coils. Change the turns ratio and the secondary voltage and current shift with it. Pick what stays put no matter how the others move.
Shared flux makes the voltage ratio
When the same flux Φ threads both coils, each coil’s induced voltage is proportional to its turns. From V = N·dΦ/dt with a shared dΦ/dt, V₁/V₂ = N₁/N₂. So the turns ratio a = N₁/N₂ is the voltage ratio itself.
Power conservation flips the current ratio
An ideal transformer is lossless, so the power in comes out unchanged: V₁I₁ = V₂I₂. If the voltage becomes a times larger, the current must become 1/a times to keep the product. That is why a step-up transformer lowers the current, and why power lines ship at high voltage and low current to cut losses.
Impedance transforms by the square
A load Z₂ on the secondary looks like a²Z₂ from the primary. Since voltage is a times and current is 1/a times, the impedance seen at the primary is V₁/I₁ = (aV₂)/(I₂/a) = a²·(V₂/I₂). A transformer is thus a tool for impedance matching, not only voltage and current.
Back to the first screen
However you turned the ratio, what stayed conserved was power. The shared flux rescales voltage by the ratio of turns, and the lossless transformer cancels that voltage change with an exactly opposite change in current. Raise the voltage by a and the current falls by 1/a, pinning the product VI = 200 W. A transformer leaves power untouched and only swaps the pairing of voltage and current.
The turns-ratio transformation is the backbone of power systems. Real transformers depart from this ideal through leakage flux, magnetising current and core and copper losses. The next unit captures that departure in an equivalent circuit to compute efficiency and voltage regulation (MC-A4). The same shared-flux principle carries into the stator–rotor coupling of induction and synchronous machines.