65.66_Applications of Electromagnetic Induction

  • ppt
  • 08.05.2020
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Lesson Objectives

By the end of the lesson learners will be able:

10.4.2.3 – to explain the operating principle of electromagnetic devices (electromagnetic relay, generator and transformer);

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Keywords

English

Russian

Kazakh

Direct current

Alternating current

Commutator

generator

induction

Motor

Slip rings

Split rings

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Glossary

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5

Now I understand!
AN EMF IS ONLY INDUCED WHEN THERE IS RELATIVE MOTION BETWEEN A CONDUCTOR AND A MAGNETIC FIELD

Voltage and Current Size

The induced Emf,ℇ, (and current, I,) is increased if:

the magnet and/or coil is moved faster (V)
there are more turns (N) on the coil
using a magnet with a stronger field (B)
A coil of several turns instead of a wire is used

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THE INDUCED EMF IS
DIRECTLY PROPORTIONAL TO
THE RATE OF CHANGE OF MAGNETIC FLUX CUTTING THE CONDUCTOR

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Induced Voltage and Inductance

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Laws of EM Induction

Faraday

Size of the voltage

Lenz

Direction of the voltage

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Note Well

 

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An EMF……..When:

IS INDUCED

The coil is moved through the magnetic field, across the pole pieces.

The magnet is moved so that the wire passes across the face of the pole pieces.

IS NOT INDUCED

The wire is held stationary between the pole-pieces.

The magnet is moved so that the pole –pieces move along the length of the wire

The wire moves lengthways so that it does not change its position between the poles of the magnet.

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LENZ’S LAW

THE INDUCED EMF GENERATES A CURRENT THAT SETS UP A MAGNETIC FIELD WHICH ACTS TO OPPOSE THE CHANGE IN MAGNETIC FLUX

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Activity

Explain the applications of electromagnetic induction in:
Electromagnetic relay
Simple generator
Transformer
Metal detector

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B

FLEMING’S RIGHT HAND RULE

conductor

MOTION

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Fleming’s Left and Right Hand Rules

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POTENTIAL DIFFERENCE GENERATED ACROSS A MOVING CONDUCTOR

E = B L v

B INWARDS

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If the wingspan is L
E = B L v cos θ

Potential Difference across wing tips of an aircraft moving through the Earth’s magnetic field acting at 200 to the vertical.

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Sound waves strike the diaphragm making it vibrate at the same frequency as the sound. The moving diaphragm moves the coil backwards and forwards which induces a changing current at the same frequency as the sound.

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PRIMARY N1 Turns
AC input V1 Volts

SECONDARY N2 Turns
AC output V2 Volts

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METAL DETECTOR

This acts like a transformer. AC current is sent through circular coil (field coil) which is down near the ground. If a metal is underneath the coil, an eddy current will be set up in it. This will have an associated magnetic field which in turn will affect the AC current in the field coil. The change is detected electronically.