induced voltages and inductance chapter 20 hans christian oersted

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Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

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Page 1: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Induced Voltages And Inductance

Chapter 20

Hans Christian Oersted

Page 2: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Introduction Oersted’s discovery was the first evidence of a link between electricity and magnetism.

Page 3: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Symmetry in Physics Symmetry in nature helps scientists to make new discoveries.

Page 4: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Generating Electricity Could magnetic fields produce electric currents? Joseph Henry made this discovery

Power plants were the result of his efforts

Page 5: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Induced emf And Magnetic Flux

Faraday’s experiment A current can be produced by a changing magnetic field.

20.1

Page 6: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Primary and Secondary Coils

A steady magnetic field in the primary coil cannot produce a current in the secondary coil.

Page 7: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Induced emf And Magnetic Flux

Magnetic flux The flux is proportional to the number of lines passing through the loop

Changes in the flux induce a change in the emf.

20.2

Page 8: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Magnetic Flux Formula

is the angle between the B field and

the normal to the plane of the loop

=BA = BAcosθ

Page 9: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Faraday’s Law of Induction

A simple demonstration Wire loop, galvanometer, magnet

20.4

Page 10: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Induced Current A current is set up in the loop as long as there is relative motion between the magnetic field and the loop. This is an induced current.

20.4

Page 11: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Faraday’s Law of Induction

The induced emf () in a circuit equals the rate of change of the magnetic flux through the circuit.

Page 12: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Formula for Faraday’s Law of magnetic induction

=−NΔΦB

Δt

Page 13: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Faraday’s Law of Induction

SinceA.cos

And = -N./t

Then = -N.A.cos/t

Page 14: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Lenz’s Law The induced current tries to maintain the original flux through the circuit. It sets up a magnetic field that opposes any change in the original magnetic field.

Page 15: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted
Page 16: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Applications of Faraday’s Law

Electric guitar Metal strings Pickup coil

Cruise control Ground fault interrupter (GFI)

Protects against electrical shock Where is it used? How does it work?

SIDS monitor

20.10a, 209, 20.8, 214, 20.5

Page 17: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Motional emf Motional emf is the emf induced in a conductor moving through a magnetic field. Example: A straight conductor moving through a magnetic field

20.8, 20.13

Page 18: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Formula:

V = El = Bl v

Page 19: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Motional emf A potential difference (V) is maintained across a conductor as long as there is motion through the field. If the direction of the motion is reversed, the polarity also reverses.

Page 20: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Motional emf Motion involving a closed conducting path Current flows through the circuit

162, 211

Page 21: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Important Formulas:

=t

= Bl v

I =ε

R=Bl v

R

Page 22: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Lenz’s Law Revisited Another example (Figure 20.17): A stationary conducting loop and a bar magnet

215, 20.13, 165

Page 23: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Applications of Magnetic Induction

Cassette tape recorders/players Magnetic tape Recording head Playback head

VHS recorders/players Computer hard drives

Page 24: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Questions

1 - 7

Pg. 689

Page 25: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

AC Generators The alternating current (ac) generator

Converts mechanical energy to electrical energy

Has a coil rotating in a magnetic field Slip rings

Insure that the output voltage changes polarity Stationary brushes

20.20, 216

Page 26: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Types of Commercial Power Plants

Fossil Fuel Hydroelectric Nuclear

Page 27: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Total emf Formula for total emf:

Notet = andf (f = 60 Hz in USA)

is measured between the magnetic field and the normal to the loop.

Maximum emf occurs when the plane of the loop is parallel to the magnetic field

213

=NBAω sin(ωt)

Page 28: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

DC Generators The direct current (dc) generator Uses a split ring or commutator

This insures that the output voltage does not change polarity.

20.22

Page 29: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Motors and Back emf A motor is the opposite of a generator. Because of Lenz’s Law, back emf is generated in a motor.

Back emf increases with rotational speed. Back emf tends to reduce current flow in the windings.

Maximum current is present when the motor starts up.

217

Page 30: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Back emf vs. Speed

Page 31: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Equation for back emf

=V − I ⋅R

Page 32: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Eddy Currents Eddy currents are circular currents which occur in a piece of metal when it moves through a magnetic field

Page 33: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Magnetic Damping The magnetic fields produced by the eddy currents try to prevent motion of the metal through the field.

Page 34: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Effects of Eddy Currents

The effects of eddy currents are undesirable in motors and generators. These effects can be reduced

Laminations are used

Page 35: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Laminations in an Armature

Page 36: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Self-Inductance A changing flux through the circuit arises from the circuit itself. This occurs in coils and solenoids

Solenoid Video

Page 37: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Self-Induced emf The self induced emf is proportional to the time rate of change of current

L is a constant representing the inductance of the device and is measured in Henries (H).

=−LΔI

Δt

Page 38: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Inductance Formula for inductance (L)

L =μoN

2A

l€

L =NΔΦ

ΔI

Page 39: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Inductors An inductor is a circuit element which is used to provide inductance.

Usually a closely wrapped coil of many turns

Page 40: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Inductance Inductance (L) is a measure of the opposition to the rate of change of current. Schematic symbol

20.27/20.28

Page 41: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

RL Circuits RL time constant ()

The time that it takes for the current in the circuit to reach 63.2 % of its maximum value.

=L

R

Page 42: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Energy Stored In A Magnetic Field

Current flowing through a solenoid produces a magnetic field. The battery must do work to produce a current in a coil.

This energy is stored in the magnetic field of the coil.

37-1, 14, 78

PEL = 1

2LI2

Page 43: Induced Voltages And Inductance Chapter 20 Hans Christian Oersted

Questions

8,10, 11, 13, 14

Pg. 689