Difference between revisions of "Back EMF"

Revision as of 09:30, 22 May 2024

Back emf is the electromotive force (emf) induced in the spinning coil of an electric motor or in any coil where the current is changing, such as in the primary coil of a transformer. This back emf acts against the change of applied potential difference (pd).

Back emf occurs due to Lenz's Law, which states that the direction of the induced emf is such that it opposes the change causing it.
In an electric motor, back emf increases with the speed of the motor.
It limits the current flowing through the motor as the speed increases.
In transformers, back emf is induced in the primary coil when the current in the secondary coil changes.
Back emf is crucial for the functioning of devices like motors and transformers by preventing excessive currents.
It is a key factor in the design and operation of AC and DC motors.

When an electric motor starts, the back emf is initially zero, allowing maximum current.
Back emf in transformers helps regulate the current and voltage during operation.

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 *[[Back EMF|Back emf]] occurs due to [[Lenz's Law|Lenz's Law]], which states that the direction of the [[Electromagnetic *Induction|induced]] [[Electromotive Force|emf]] is such that it opposes the change causing it.
-*In an [[Motor|electric motor]], back [[Electromotive Force|emf]] increases with the [[speed]] of the [[motor]].
+*In an [[Motor|electric motor]], [[Back EMF|back emf]] increases with the [[speed]] of the [[motor]].
 *It limits the current flowing through the motor as the [[speed]] increases.
 *In [[Electrical Transformers|transformers]], [[Back EMF|back emf]] is [[Electromagnetic *Induction|induced]] in the [[Primary Coil|primary coil]] when the [[Electrical Current|current]] in the [[Secondary Coil|secondary coil]] changes.