Circuits & Electrical Power · The solenoid
The field a coil builds
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The field a coil builds

Wind a wire into a long tight helix, push a current through it, and the field inside comes out remarkably uniform — that is a solenoid, and it is the working heart of every relay, contactor and solenoid valve you will ever meet. Its field is B=μ0NILB = \dfrac{\mu_0 N I}{L}, read aloud B equals mu-nought N I over L.

The letters. BB is the field inside the coil in tesla. NN is the total number of turns — a plain count, no units. II is the current in amperes. LL is the length of the coil in metres, end to end along its axis. And μ0\mu_0 is the permeability of free space, 4π×107 Tm/A4\pi\times 10^{-7}\ \mathrm{T\cdot m/A} — a constant, like gg, that comes free with the universe. Turns, current and length are given here; BB is what you solve for.

Here is the distinction the whole lesson turns on. Textbooks often write the same law as B=μ0nIB = \mu_0 n I, and that nn is not NN. Little nn is N/LN/L, the turns per metre, measured in m1\mathrm{m^{-1}}; big NN is the bare count. Confuse them and your answer is wrong by a whole factor of the coil's length — which, for a 20 cm coil, means five times too big. Think of it physically: take a finished coil and stretch it out to twice the length without adding a single turn, and the field inside halves. Nothing about NN changed. Everything about nn did.

Units guide, they do not confess. Push them through: Tm/A\mathrm{T\cdot m/A} times amps, divided by metres, leaves tesla — the rearrangement survives. If the units refuse to land on tesla the algebra is wrong, no appeal. But units that do work out never prove you right; the check runs one way only.