 Download Presentation Lesson 9

# Lesson 9 - PowerPoint PPT Presentation

Lesson 9. Lesson 9. Faraday’s Law. Faraday’s Law of Induction Motional EMF Lenz’s Law Induced EMF’s and Induced Electric Fields Eddy Currents. Torque on Loop. Current in loop in a magnetic field produces torque on a loop. Induced Current. I am the owner, or an agent authorized to act on behalf of the owner, of the copyrighted work described.
Download Presentation ## Lesson 9

An Image/Link below is provided (as is) to download presentation

Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author.While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server.

- - - - - - - - - - - - - - - - - - - - - - - - - - E N D - - - - - - - - - - - - - - - - - - - - - - - - - -
Presentation Transcript Lesson 9

Lesson 9

• Faraday’s Law of Induction
• Motional EMF
• Lenz’s Law
• Induced EMF’s and Induced Electric Fields
• Eddy Currents Torque on Loop

Current in loop in a magnetic field produces torque on a loop Induced Current

Does torque on loop in a magnetic field produces current in a loop ?

YES Picture

I

B

• current depends on the torque
• thus on rotational frequency Change of Flux Picture
• Current depends on speed of magnet
• Thus rate of change of magnetic Field Change of Flux Picture Equations

Common factors, change of area, change of magnetic field Induced Current in Wire

moving wire in field B produces current I if there is a conduction path

I

B

v

FB Induced emf

(y,

z1)

(y,

z2)

y1

k

j

i  Equations II

Work done per unit charge by

F

B

in moving charges from

z

to

z

1

2

=

vBl

where

l

=

z

-

z

2

1

No work is done in moving charges in

other sections of path

(

ignore Hall effect

)

dW

Work done per unit charge

=

emf

dQ

Thus

e

=

vBl Equations III

Area of loop in magnetic field

(

)

(

)

(

)

A

t

=

y

t

-

y

l

1

Total magnetic flux through loop

(

)

F

t

Rate of change of magnetic flux

e

d

F

dy

=

-B

l

=

-

Bvl

=

-

dt

dt s Law of Induction for N loops  '

Faradays Law of Electromagnetic Induction

The work done per unit charge by magnetic force

moving charge from

z

to

z

1

2

ò

ò

ò

z

2

dW

1

1

=

·

=

·

=

·

F

s

F

s

E

s

d

d

d

B

B

ind

dQ

Q

Q

z

loop

loop

1

thus

ò

e

F

d

=

-

=

·

d

E

s

N

ind

dt

loop Induced Electric Field
• An induced EMF is a measure of
• An induced Electric Field
• If charge is in this region and there is a conduction path it will feel a force from the induced Electric Field and flow Equations

E

Remember for a static electric field

stat

ò

b

=

·

E

s

V

d

and

ab

stat

a

ò

=

·

=

E

s

E

d

0

as

is conservative

stat

stat

E

But for an induced electric field

ind

ò

·

¹

E

s

d

0

ind

thus

E

is not conservative

ind Magnetic Flux and Induced Electric Field

Changing Magnetic Flux produces an

Induced Electric Field Mechanical Work to Electrical work I

Pulling at constant velocity v

B

v

l

Fappl

I

Blv

y

k

j

i Mechanical Work to Electrical work II

l

wire

with current I flowing in it

B

moving in a magnetic field

feels a force given by

=

´

F

l

B

I

=

-

´

=

-

F

k

i

j

IlB

IlB

F

This force opposes the applied force

appl

and must be equal and opposite if the

velocity is to remain constant

=

=

F

F

IlB

appl   Mechanical Power to Electrical Power II

Pulling at constant velocity v

B

v

F

l

Fappl

I

Blv Magnetic Field produced by Changing Current

Circulating current produces an induced magnetic field

I

Bind

That opposes the external magnetic field B

That produces the current Current produced by Changing Magnetic Field

(a) Change of External Magnetic Field Produces Current

(b) Current Produces Induced Magnetic Field Lenz's Law

Lenz’s Law

Polarity of is such that

it opposes the change that caused it

Direction of Eis such that

it opposes the change that caused it

Direction of induced current is such that

it opposes the change that caused it Conservation of Energy

Conservation of Energy AC Generator

AC Generator e

AC Potential

F

d

d

(

)

(

)

=

-

=

-

·

B

A

t

dt

dt

d

(

)

(

)

=

-

=

q

BACos

BA

sin

d

q

(

t

)

q

t

dt

dt

if rotational speed is constant

e

e

(

)

(

)

(

)

w

w

t

wBA

sin

t

sin

t

=

=

max

e

=

BAw

max DC Generator

DC Generator 