eleanor roosevelt high school chin-sung lin lesson 21

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Electromagnetic Induction Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

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Page 1: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Electromagnetic Induction

Eleanor Roosevelt High SchoolChin-Sung Lin

Lesson 21

Page 2: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Electromagnetic Induction & Faraday’s Law

Page 3: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

In 1831, Michael Faraday (England) and Joseph Henry (US) independently discovered that magnetism could produce current in a wire

Electromagnetic Induction

Page 4: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Faraday’s law— Electromagnetic induction

Electromagnetic induction— any change in the magnetic field around a conductor induces a voltage (or emf)

Faraday’s law— The induced voltage (or emf) in a coil is proportional to the product of the number of loops and the rate of change of the magnetic field within those loops

Electromagnetic Induction

Page 5: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

How can we change the magnetic field around a conductor to induces a voltage (or emf)?

Electromagnetic Induction

Page 6: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

The change could be produced by

◦ relative motion of a wire with respect to the magnetic field

Electromagnetic Induction

Page 7: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

The change could be produced by

◦ moving the coil into or out of the magnetic field

Electromagnetic Induction

Page 8: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

The change could be produced by

◦ rotating the coil relative to the magnet

Electromagnetic Induction

Page 9: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

The change could be produced by

◦ changing the magnetic field strength

Electromagnetic Induction

Page 10: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

A magnet moving past a stationary conductor, or

A conductor moving through a stationary magnetic field

Electromagnetic Induction

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The work done to the magnet is equal to the energy generated in the circuit to which the coil is connected

Wmechanical = Welectric

Electromagnetic Induction

Page 12: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Induced voltage depends on:

◦Speed of the wire traversing the magnetic field lines. Quicker motion induces a greater voltage (V ~ v)

◦Number of loops of wire that moves in a magnetic field. The voltage is proportional to the number of loops (V ~ N)

Induced Voltage

Page 13: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

If the coil does not form a complete circuit, what will happen?

Induced Voltage

Page 14: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Induced voltage without current, no work to plunge the magnet into the coil

Induced Voltage

-+

Page 15: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

If the coil forms a complete circuit, what is the direction of the induced current?

Induced Current

A

Ammeter

Page 16: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

The induced magnetic field is repelling, the current will flow in a way to create such a repelling field

Induced Current

A

Ammeter

Page 17: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

The more loops of the coil, the more voltage induced (V ~ N)

The more voltage induced in the coil, the more current through the resistor in the circuit (I ~ V)

The more current through the coil, the stronger the magnetic field it generated (B ~ I)

The stronger the magnetic field generated, the stronger the repelling force acting back to your magnet (F ~ B)

A coil with more loops is a stronger electromagnet and push back harder

Induced Current

Page 18: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

What factors will affect the induced current?

Induced Current

A

Ammeter

Page 19: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Induced current depends on ◦the induced voltage ◦the resistance of the coil and the◦the “reactance” of the coil

Induced Current

Ammeter

A

Page 20: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Reactance

◦similar to resistance ◦depends on the number of loops in the coil the frequency of the AC source

Reactance

Page 21: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Reactance

The counter-emf is the source of the opposition to current flow change

◦A constant DC current has a zero rate-of-change, and sees an inductor as a short-circuit

◦An AC current has a time-averaged rate-of-change that is proportional to frequency, this causes the increase in inductive reactance with frequency

Reactance

Page 22: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Induced voltage of a moving conductor in a magnetic field

V = v B L

Moving Conductor in a Magnetic Field

Page 23: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Generators &Alternating Current

Page 24: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

The movement of a magnet is alternating, the induced voltage alternates on direction

The greater the frequency of the field change, the greater the induced voltage

Generator & Alternating Current

Page 25: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

The frequency of the induced alternating voltage equals the frequency of the alternating magnetic field within the loops

Generator & Alternating Current

High Frequency

Low Frequency

Page 26: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Generator— a device that converts mechanical energy to electrical energy

Motor— a device that converts electrical energy to mechanical energy

Generator & Alternating Current

Page 27: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

When a closed conductor loop is moved in a magnetic field, an induced current flows through it

The direction of induced current is given by the Flemming's right hand generator rule

Flemming’s Right Hand Generator Rule

Page 28: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Generator & Alternating Current

What’s the direction of the induced current?

N

S

Page 29: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Generator & Alternating Current

Given by the Flemming's right hand generator rule

N

S

Page 30: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Generator & Alternating Current

As the number of magnetic field lines within the loop changes, the magnitude and direction of the induced voltage and current change

Page 31: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Generator & Alternating Current

Page 32: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Generator & Alternating Current

One complete rotation of the loop produces on complete cycle in voltage and current

Page 33: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Generator & Alternating Current

The voltage induced by the generator alternates, and the current produced is alternating current (AC)

The standard alternating current is 60 Hz

Page 34: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Generator Example

Hydro power generators

Page 35: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Aim: Transformer & Electromagnetic WaveDoNow: Draw the voltage waveform

One complete rotation of the loop produces on complete cycle in voltage and current

Page 36: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Aim: Transformer & Electromagnetic WaveDoNow: Draw the voltage waveform

One complete rotation of the loop produces on complete cycle in voltage and current

Page 37: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Transformers

Page 38: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Transformer Definition

A a static device that transfers electrical energy from one circuit to another through inductively coupled conductors

A static device that transfers electrical energy to magnetic energy, and to electric energy again

A device with which we can raise (for transmission) and lower (for use) the AC voltage in a circuit

Transformer only works for AC

Page 39: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Transformer Principle

Primary

Secondary

Primary and secondary coils Use AC voltage source (primary coil) AC voltage is induced (secondary coil) Frequency AC voltage source = Frequency Induced AC voltage

Page 40: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Transformer Principle

Iron core (high permeability) is inserted into the coils to intensify the magnetic field

Iron core forms a complete loop to guide all magnetic field lines through the secondary

Page 41: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Transformer Principle

Transformer Symbol:

Page 42: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Transformer Principle

Np no. of turns of primary coil

Ns no. of turns of secondary coil

Vp voltage of primary coil

Vs voltage of secondary coil

Ip current of primary coil

Is current of secondary coil

IPIS

Page 43: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Transformer Principle

IP

IS

VP VS

NP NS

=

Page 44: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Transformer Principle

Step-up transformer◦NP < NS

◦VP < VS

Step-down transformer

◦NP > NS

◦VP > VS

Page 45: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Transformer Principle

IP

IS

PP = PS

IP VP = IS VS

Page 46: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

VP / NP = VS / NS

IP VP = IS VS

VP / VS = IS / IP = NP / NS

VS = VP (NS / NP )

IS = IP (NP / NS )

Transformer Principle

VP IS NP

VS IP NS

= =

NS

NP

VS = VP

NP

NS

IS = IP

Page 47: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Application - Power Transmission

Page 48: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Electromagnetic Waves

Page 49: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Induction of Electric Field Faraday’s law:

◦ An electric field is created in any region of space in which a magnetic field is changing with time

◦ The magnitude of the created electric field is proportional to the rate at which the magnetic field changes

◦ The direction of the created electric field is at right angles to the changing magnetic field

Page 50: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Induction of Magnetic Field Maxwell’s law:

◦ A magnetic field is created in any region of space in which an electric field is changing with time

◦ The magnitude of the created magnetic field is proportional to the rate at which the electric field changes

◦ The direction of the created magnetic field is at right angles to the changing electric field

Page 51: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Electromagnetic Waves In 1861 Scottish physicist

James Clerk Maxwell discovered the theory of electromagnetism

Maxwell united all previously unrelated observations and equations of electricity, magnetism and optics into a consistent electromagnetic field theory

Page 52: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Electromagnetic Waves German physicist Heinrich

Rudolf Hertz was the first to satisfactorily demonstrate the existence of electromagnetic waves by building an apparatus to produce and detect VHF or UHF radio waves

Page 53: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Electromagnetic Waves A charge oscillates back and forth in empty

space will produce electromagnetic waves in space where vibrating electric and magnetic fields regenerate each other

Page 54: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Electromagnetic Waves Electric field is perpendicular to the

magnetic field, and both are perpendicular to the direction of the motion of the wave

Page 55: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

Electromagnetic Waves No medium is required The speed— the speed of light The wave is continuously self-reinforcing. The

changing electric field induced a magnetic field. The changing magnetic field acts back to induce a electric field

Page 56: Eleanor Roosevelt High School Chin-Sung Lin Lesson 21

The End