Electric Motor Diagram: How AC and DC Motors Work

Every motor -- from a tiny computer cooling fan to a 500 kW pump motor -- converts electrical energy into mechanical rotation using the same basic principle: a current-carrying conductor in a magnetic field experiences a force. What varies between motor types is how the magnetic field is produced and how the current is commutated to keep the rotation continuous. This guide covers the internal structure of both AC induction motors and DC motors, with labeled diagrams of the key components and how they produce torque.

The Common Principle: Lorentz Force

A conductor carrying current I in a magnetic field B experiences a force F:

F = BIL

where L is the length of the conductor. In a motor, the current-carrying conductors are wound onto a rotating assembly (the rotor). The fixed magnetic field is created by the stationary assembly (the stator). The force on the rotor conductors creates a torque that turns the shaft.

In practice, getting that torque to continue in one direction -- rather than just pulling the rotor to alignment and stopping -- requires either commutation (DC motors) or a rotating magnetic field (AC induction motors).

DC Motor Diagram

Main Components

Stator (field assembly) The stator of a wound-field DC motor consists of:

Rotor (armature)

End shields / end bells Cast metal end plates that hold the rotor bearings and brush holders.

How a DC Motor Produces Rotation

  1. Current enters the motor through the positive brush, flows through the commutator segment in contact, and into the armature winding.
  2. The conductor in the magnetic field experiences the Lorentz force -- in this diagram, the force on the top conductor is toward the viewer (using the right-hand rule: field pointing left, current going away from viewer → force upward then curving into the page).
  3. This force creates a torque that begins to rotate the armature.
  4. As the armature turns approximately 90°, the commutator segments shift contact to the next brush. The current direction in the same physical conductors reverses -- but they are now on the other side of the poles, so the force direction in space remains the same.
  5. This commutation continues, maintaining continuous torque in one direction.

DC Motor Types and Their Wiring Diagrams

Permanent Magnet DC (PMDC): Two external terminals -- positive and negative. Reversing polarity reverses rotation. Used in toys, power tools, actuators.

Series DC motor: Field winding in series with the armature. Very high starting torque, speed varies dramatically with load. Used in traction, cranes, and historically in starter motors.

Shunt DC motor: Field winding in parallel with the armature (both connected across the same supply). Nearly constant speed with varying load. Used in machine tools and fans.

Compound DC motor: Both series and shunt field windings. Combines high starting torque with better speed regulation than a pure series motor.

AC Induction Motor Diagram

The three-phase squirrel cage induction motor is the most common motor in industrial use -- it has no brushes, no commutator, and no electrical connection to the rotor. It is also the motor covered in the 3-phase motor wiring diagram guide (terminal box connections, star/delta wiring).

Main Components

Stator

Rotor

Shaft, bearings, and frame: Same general construction as a DC motor.

How an AC Induction Motor Produces Rotation

  1. The three-phase stator windings produce a rotating magnetic field that spins at the synchronous speed: Ns = 120f / P, where f is supply frequency (60 Hz in US) and P is the number of poles.

    • For a 2-pole motor at 60 Hz: Ns = 120 × 60 / 2 = 3,600 RPM
    • For a 4-pole motor at 60 Hz: Ns = 1,800 RPM
    • For a 6-pole motor at 60 Hz: Ns = 1,200 RPM
  2. The rotating magnetic field sweeps past the stationary rotor bars. By Faraday's law, the changing flux induces a voltage in the short-circuited rotor bars, causing a rotor current to flow.

  3. The rotor current is in a magnetic field (the stator's rotating field). Lorentz force acts on the rotor bars, creating torque. The rotor accelerates in the direction of the rotating field.

  4. The rotor never reaches synchronous speed. If it did, there would be no relative motion between the field and the rotor bars, no induced EMF, no rotor current, and no torque. The rotor always lags the rotating field by the slip: s = (Ns - Nr) / Ns. At full load, slip is typically 2 to 5%.

Single-Phase Induction Motor

Single-phase AC does not create a rotating field -- it creates a pulsating field. A single-phase motor cannot start on its own because the pulsating field produces zero net torque at standstill. A starting method is required:

Comparing AC Induction and DC Motor Diagrams

Feature DC Motor AC Induction Motor
Rotor connection External (via brushes and commutator) None (inductively coupled)
Speed control Easy -- vary armature voltage Needs VFD for smooth speed control
Starting torque Very high (especially series) Moderate (6--8x FLC inrush)
Maintenance Brushes and commutator wear Bearings only
Efficiency Good, but brush losses High, especially larger sizes
Cost Higher (more complex construction) Lower

Torque-Speed Characteristic

For a DC shunt motor, torque is nearly proportional to armature current, and speed drops slightly with load -- a relatively flat speed curve.

For an AC induction motor, the torque-speed curve has a characteristic hump at the breakdown torque point (typically 200 to 300% of rated torque) before the motor accelerates through to the running region near synchronous speed. Understanding this curve is important when selecting a motor for high-inertia loads.

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Key Takeaways