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Counter-electromotive force

From Wikipedia, the free encyclopedia
(Redirected fromBack EMF)
Voltage that opposes the change in current which induced it

Inelectromechanics, thecounter-electromotive force (also calledcounter EMF,CEMF orback EMF),[1] is the opposingelectromotive force (EMF) caused by a changing current. The changing current leads to a changing magnetic field, and hence induces a EMF in the circuit byFaraday's law of induction.

Details

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For example, the voltage appearing across aninductor orcoil is due to a change in current which causes a change in themagnetic field within the coil, and therefore the self-induced voltage.[1][2] Thepolarity of the voltage at every moment opposes that of the change in applied voltage, to keep the current constant.[1][3]

The termback electromotive force is also commonly used to refer to the voltage that occurs inelectric motors where there is relative motion between thearmature and the magnetic field produced by the motor'sfield coils or permanent magnet field, thus also acting as a generator while running as a motor. This effect is not due to the motor's inductance, which generates a voltage in opposition to a changing current via Faraday's law, but a separate phenomenon. That is, the back-EMF is also due to inductance and Faraday's law, but occurs even when the motor current is not changing, and arises from the geometric considerations of an armature spinning in a magnetic field.

This voltage is in series with and opposes the original applied voltage and is called "back-electromotive force" (byLenz's law). With a lower overall voltage across the motor'sinternal resistance as the motor turns faster, the current flowing into the motor decreases.[4] One practical application of this phenomenon is to indirectly measure motor speed and position, as the back-EMF is proportional to the rotational speed of the armature.[5]

In motor control and robotics, back-EMF often refers most specifically to actually using the voltage generated by a spinning motor to infer the speed of the motor's rotation, for use in better controlling the motor in specific ways.[6]

To observe the effect of back-EMF of a motor, one can perform this simple exercise: with an incandescent light on, cause a large motor such as a drill press, saw, air conditioner compressor, or vacuum cleaner to start. The light may dim briefly as the motor starts. When the armature is not turning (called locked rotor) there is no back-EMF and the motor's current draw is quite high. If the motor's starting current is high enough, it will pull the line voltage down enough to cause noticeable dimming of the light.

References

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  1. ^abcGraf, "counterelectromotive force", Dictionary of Electronics
  2. ^Griffiths, David J. (2023).Introduction to Electrodynamics (5th ed.). Cambridge University Press. pp. 325–331.doi:10.1017/9781009397735.ISBN 978-1-009-39773-5.
  3. ^"Self-Inductance,"Naval Electrical Engineering Training Series, Module 02: Introduction to Alternating Current and Transformers.Archived 2006-04-20 at theWayback Machine
  4. ^"Nuclear Power Fundamentals Training Manuals". DC Generators,Counter-Electromotive ForceArchived 2007-09-29 at theWayback Machine (CEMF), DC Equipment Terminology, Electrical Science Volume 2.
  5. ^"Back-EMF". Acroname.com. 2006-08-07. Retrieved2010-02-07.
  6. ^"Back EMF Motion Feedback"Back EMF Motion Feedback[permanent dead link]

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