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An AC motor converts alternating current electrical energy into mechanical rotational energy through the principle of electromagnetic induction. When AC supply voltage is applied to the stator windings, it generates a rotating magnetic field (RMF). The speed at which this field rotates is called the synchronous speed, determined by the supply frequency and the number of magnetic pole pairs in the stator: Ns = 120f / P, where f is supply frequency in Hz and P is the number of poles.
In an induction motor — the most common AC motor type — the rotating magnetic field cuts across the rotor conductors and induces a current within them by Faraday's law. That induced current produces its own magnetic field, and the interaction between the rotor field and the stator's rotating field generates a torque that drives the rotor to spin. The rotor always runs slightly slower than the synchronous speed; this speed difference is called slip, typically 2–8% in standard induction motors. Without slip, no relative motion exists between the field and rotor conductors, no current is induced, and no torque is produced.
In synchronous AC motors, the rotor is instead excited by a DC field or uses permanent magnets, locking it to rotate at exactly synchronous speed with zero slip. This makes synchronous motors the preferred choice where precise constant-speed operation is critical, such as in clock mechanisms, certain textile machinery, and high-efficiency variable-speed drives.

Understanding the internal architecture of an AC motor helps with specifying the right unit, diagnosing faults, and planning maintenance intervals. The major components are:
Additional components present in specific motor types include slip rings and brushes (wound-rotor induction motors), centrifugal starting switches (single-phase capacitor-start motors), and capacitors (single-phase run-capacitor and capacitor-start/run designs).
AC motors divide into two primary families — induction (asynchronous) and synchronous — each with several subtypes optimized for different operating requirements.
| Motor Type | Supply | Key Characteristic | Typical Applications |
|---|---|---|---|
| Squirrel-cage induction | 3-phase | Simple, robust, low maintenance; runs with slip | Pumps, fans, compressors, conveyors |
| Wound-rotor induction | 3-phase | External rotor resistance allows high starting torque and speed control | Cranes, hoists, large mills |
| Permanent magnet synchronous (PMSM) | 3-phase (via VFD) | High efficiency (IE4/IE5), no rotor copper loss, runs at synchronous speed | HVAC, servo drives, EV traction |
| Capacitor-start induction | Single-phase | Capacitor in series with start winding creates phase shift for starting torque | Air compressors, refrigeration, pumps |
| Capacitor-start / capacitor-run | Single-phase | Two capacitors: one for starting, one for running; higher efficiency than capacitor-start only | Woodworking machinery, power tools |
| Shaded-pole motor | Single-phase | Very simple construction, low starting torque, low efficiency | Small fans, appliances, vending machines |
| Reluctance synchronous | 3-phase (via VFD) | No rotor windings or magnets; torque produced by rotor saliency; IE4-capable | Industrial pumps, fans with VFD |
For the majority of industrial applications, the three-phase squirrel-cage induction motor remains the default choice. It requires no brushes, slip rings, or external excitation, making it the lowest-maintenance and most cost-effective option for constant-speed loads. Variable-frequency drives (VFDs) have extended its usability to variable-speed applications that previously required DC or wound-rotor motors.
Wiring an AC motor correctly is essential for safe operation and achieving the correct torque and speed characteristics. The terminal box configuration varies by motor type and supply voltage, but the following covers the most widely encountered scenarios.
Most three-phase induction motors are wound for two voltage levels — commonly 230V/400V or 400V/690V — and the terminal box contains six leads labeled U1, V1, W1 (winding starts) and U2, V2, W2 (winding ends). The supply voltage determines the connection:
Star-Delta starting is a common soft-start method for large motors: the motor starts in star (reduced voltage across each winding = lower starting current, typically 1/3 of direct-on-line inrush), then switches to delta once it approaches full speed. This reduces supply disturbance but also reduces starting torque by the same 1/3 factor, so it is only suitable for low-load starting applications.
Single-phase AC motors require an auxiliary starting circuit because a single-phase supply alone cannot produce a rotating magnetic field. The terminal arrangement typically includes:
Reversing the direction of rotation of a three-phase motor requires swapping any two of the three supply phases at the motor terminals — for example, exchanging the connections at U1 and V1. This reverses the direction of the rotating magnetic field and consequently the rotor. For single-phase motors, reversal is achieved by swapping the start winding connections relative to the main winding; some motors provide dedicated terminal markings for this purpose, while others require internal reconnection.
Every AC motor installation must include a protective earth (PE) connection bonded to the motor frame, connected to the supply earth at the terminal box. In addition, a properly rated thermal overload relay or electronic motor protection relay should be installed in the supply circuit, set to the motor's full-load current (FLC) rating. Overload protection is the primary defense against the most common motor failure mode: prolonged overcurrent from mechanical overload, single-phasing, or restricted ventilation that elevates winding temperature beyond the insulation class limit.
