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ENSC2003 - Lecture 17
DC Motors - Slides
DC Motors Y12

DC Motors

  • Motor converts electrical energy into mechanical energy
  • Generator converts mechanical energy to electrical energy

  • Rotor rotating part of motor
    • Carriers wire-wound coils
    • Coils create Lorentz force when energised
  • Stator stationary part of motor
    • Holds magnets that create a fixed field

Circuit Model of DC Motors

The conduction path of the motor looks like:

  • Brush -> commutator -> coils -> commutator -> brush

There are only three important properties we need to model:

  1. armature resistance
    • i.e. the wire resistance in the coils
  2. armature inductance
  3. back-EMF
    • Generated by coils spinning in magnetic field
    • Opposes the applied voltage (Lenz’s law)

DC Steady-State

From Lenz’s law:

In steady-state, inductor -> short circuit

  • Thus, we are left with two equations:
    1. Electrical:
      • Given by KVL
    2. Mechanical:
      • From torque equations

For an ideal motor, torque constant and armature constant are equal

Analogue Speed Control

Constant voltage drive

  • Motor won’t move below a threshold voltage
    • Minimum voltage:
    • This is due to static friction
  • Then, suddenly jumps to speed above the minimum
    • Thus, some speeds are inaccessible from a stationary start
    • Think of pushing a heavy box in real life

Constant current drive

  • Better torque control since

Digital Speed Control

Pulse-width modulation (PWM)

  • Voltage is either zero or a maximum value
    • Ensures voltage is always above threshold value
  • Motor drive voltage is periodic
    • On for time
    • Off for time
    • Total period is
    • Duty cycle is
  • If is sufficiently small, motor movement is continuous

PWM is the solution to the static friction problem of constant voltage sources; we can achieve any speed with good control


End of Unit!