Back EMF: Definition and Concept

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SUMMARY

Back EMF, or counter-emf, is a voltage generated in electrical windings that opposes the source voltage, thereby limiting current flow. This phenomenon arises due to Faraday’s Law and is particularly significant in applications such as variable-speed drives and permanent magnet brushless DC motors. In these motors, concentrated stator phase windings create a trapezoidal shaped back EMF, which is crucial for regulating current. Understanding back EMF is essential for optimizing the performance of motors and transformers.

PREREQUISITES
  • Understanding of Faraday’s Law of Electromagnetic Induction
  • Knowledge of electrical motor operation, specifically brushless DC motors
  • Familiarity with variable-speed drive systems
  • Basic concepts of magnetic flux and its relation to voltage generation
NEXT STEPS
  • Research the principles of Faraday’s Law in depth
  • Explore the design and operation of permanent magnet brushless DC motors
  • Learn about variable-speed drive systems and their current regulation techniques
  • Investigate the impact of back EMF on transformer efficiency and performance
USEFUL FOR

Electrical engineers, motor control specialists, and anyone involved in the design or optimization of electrical machines and drives will benefit from this discussion on back EMF.

Vishalatbatu
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Will u tell me what is back emf?
 
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Vishalatbatu said:
Will u tell me what is back emf?

Welcome to the PF.

What can you tell us about it? When does it arise? Where have you heard about it?
 
Back-emf or Counter-emf is a voltage developed in an electrical winding by Faraday’s Law that opposes the source voltage, thus limiting the current in the winding. For example,
- Often the current regulator used invariable-speed drives is unable to track the commanded current because of insufficient voltage difference between the motor back EMF and the supply.
- A permanent magnet brushless DC motor with concentrated stator phase windings. The concentrated windings create a square wave flux distribution across the air gap and a trapezoidal shaped back-EMF.
- A representation of a machine in which the stator voltage equations are modeled as a voltage source in series with a reactance (and typically a resistance). The voltage source represents the back emf present on the stator windings due to the coupling between the stator and rotor circuits.

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When a current passes through a coil wound on an iron core, it generates magnetic flux in the iron core, especially if the iron core passes through the centre of the winding and back up to the other end around the outside of the coil, without any air gaps.

This magnetic flux is now in the centre of a coil of wire and it then generates a voltage across it. It does not matter if the coil is the same one that caused the magnetic flux or another coil.

So, if it is the same coil, it will generate a voltage that opposes the original voltage. This is back EMF.
If it is a different coil, a new voltage will be generated across it. This is a transformer secondary.

Back EMF happens in some motors, too.
A motor is rotating because of a voltage across it and there is a magnetic field.
Now, you have a rotating set of coils in a magnetic field. This will cause these windings to generate a voltage which will oppose the voltage which caused the motor to rotate.
This, too, is back EMF.

In both cases, back EMF is very important as it limits the current which will flow in the transformer primary or the motor windings when the device is lightly loaded.
 
Most likely this can only be answered by an "old timer". I am making measurements on an uA709 op amp (metal can). I would like to calculate the frequency rolloff curves (I can measure them). I assume the compensation is via the miller effect. To do the calculations I would need to know the gain of the transistors and the effective resistance seen at the compensation terminals, not including the values I put there. Anyone know those values?

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