DC Motor Speed: Does it Reach Constant Rotation?

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SUMMARY

A simple DC motor reaches a constant rotational speed when the back electromotive force (back EMF) nearly equals the supply voltage, effectively limiting the armature current. Initially, when the motor is stationary, the armature current is determined by the supply voltage and winding resistance. As the motor accelerates, the back EMF increases, reducing the effective voltage and torque until a balance is achieved. This equilibrium speed is maintained as the armature current just overcomes frictional forces.

PREREQUISITES
  • Understanding of Flemming's Left Hand Rule
  • Knowledge of Lenz's Law and Faraday's Law of Electromagnetic Induction
  • Familiarity with concepts of back EMF in DC motors
  • Basic principles of electrical resistance and voltage in circuits
NEXT STEPS
  • Research the relationship between back EMF and armature current in DC motors
  • Explore the effects of load on DC motor speed and torque
  • Learn about the design and operation of brushless DC motors
  • Investigate methods for controlling DC motor speed using PWM (Pulse Width Modulation)
USEFUL FOR

Electrical engineers, hobbyists working with DC motors, and students studying electromagnetism and motor control systems will benefit from this discussion.

steve0606
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For a simple DC motor like this:

http://i1-news.softpedia-static.com/images/news2/How-Brushless-DC-Motors-Work-3.jpg

Does it reach a constant rotational speed?

I know that when a current flows through it, Flemmings Left HAnd rule causes a couple of forces that results in rotation. As this happens, its flux linkage changes and Lenz's and Faradays law says that this causes an EMF to be induced as to oppose the current produced from the p.d. from the dc power supply.

What I don't understand is how the motor would move? would it accelerate then slow down, then accelerate then slow back down etc. or would it reach an equilibrium speed?

Thanks!
 
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When stationary, there is no back emf and the armature current is defined by the supply volts and the resistance of the winding. As it speeds up, the back emf increases, gradually reducing the effective voltage to drive current through the armature and limiting the torque. In the end, the maximum speed will be reached when the armature current is just enough to overcome the friction forces and the back emf will be 'almost' the same as the supply volts (but in the opposite sense, of course).
 

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