Dashboard Deep Learning Electrical Machines Induction machines How an induction motor turns

How an induction motor turns

Stator's rotating field → induced rotor EMFs → bar currents → F = i × B → torque. Slip is what makes it work.

Freshman ~9 min

Step 1 — Stator + squirrel-cage rotor at standstill (no current yet)

0.55×
ns 1500 rpm n 0 rpm s 1.00

Reference notes

Use Next → on the narrator above to step through six configurations: from a static rotor and stator, to a fully running induction motor with steady-state slip.

The six-line elevator pitch

  1. Three-phase currents in the stator produce a rotating magnetic field at synchronous speed ns (see the synchronous chapter's first lesson).
  2. The rotor is a short-circuited cage of bars — there's no external connection to it.
  3. The stator's rotating field sweeps past the stationary rotor bars, cutting them and inducing an EMF in each bar.
  4. Because the bars are short-circuited at the ends, currents flow in them — the magnitude of those currents depends on the relative speed between the field and the bars.
  5. Each bar carries a current in the stator's flux, so it experiences a force F = i·L × B. The forces all act tangentially on the rotor, in the same sense as the field's rotation.
  6. The result is a net torque that accelerates the rotor in the direction of the rotating field. By Lenz's law, the rotor's motion reduces the relative speed → reduces the induced EMFs → reduces the current → reduces the torque — until the system settles at a steady-state slip.

Why the rotor can never quite catch the field

If the rotor ever reached synchronous speed, the field would no longer sweep past the bars at all — no flux cutting, no induced EMF, no current, no torque. The rotor would coast down due to friction, fall behind the field, and re-accelerate. So in steady state the rotor settles at a speed n slightly below ns, with a small slip:

s = (ns − n) / ns

Typical full-load slip is 2–6 %. At standstill, s = 1; at no-load, s ≈ 0 (just enough to overcome friction).

Squirrel-cage vs slip-ring rotors

Why "asynchronous"

Synchronous machines lock to ns exactly. Induction machines can't — they need slip to function. Hence the name. The slip is what generates the rotor EMF that drives the rotor current that produces the torque. No slip, no party.

Take-away. Induction motors are the workhorse of the world: 90+% of installed motor base. The mechanism is purely electromagnetic and entirely self-acting — energise the stator, the rotor knows what to do.

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