Chapter 30: Electromagnetic Induction · PHY2049: Chapter 30 5 Faraday’s Law (Law #3 of E&M) dt...
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Transcript of Chapter 30: Electromagnetic Induction · PHY2049: Chapter 30 5 Faraday’s Law (Law #3 of E&M) dt...
PHY2049: Chapter 30 2
Chapter 30: Electromagnetic Induction
PHY2049: Chapter 30 3
Subjects
Induced emfFaraday’s law (law #3 of electricity and magnetism)Lenz’s lawMotional emf
Inductance
RL circuits
Magnetic energy
Generators, transformers
PHY2049: Chapter 30 4
Electric flux
∫ ⋅= AdBΦrr
B ∫ ⋅= AdEΦrr
Magnetic flux
Surface defined by a conductive loop Closed surface
(Gaussian surface)
(N m2/C)(T m2)
Units: 1 T m2 = 1 weber = 1 Wb
θBAΦ cosB =if B is uniform and surface is flat.
Magnetic Flux
PHY2049: Chapter 30 5
Faraday’s Law (Law #3 of E&M)
dtΦdN Bε −=
emf
To avoid errorsUse Faraday’s law to calculate only the magnitude of emfUse Lenz’s law to find the direction
# of turns of the loop
Flux through the loop
PHY2049: Chapter 30 6
Same as the negative sign in Faraday’s lawLenz’s law: Direction of induced emf is such that resulting current opposes change in ФB.
Let’s examine three ways to change ФB through a coil
Change BChange area of the coil (motional emf)Change angle θ of the coil with respect to B (motional emf) – principle of the generator
Lenz’s Law
PHY2049: Chapter 30 7
Q1 Is the induced emf and current clockwise or counterclockwise?
Q2 What does the ammeter read, when the magnet is held in place?
Clockwise
ZeroQ3 What happens while the magnet is being pulled back? Counterclockwise emf and currentQ4 What happens if the S pole of the magnet is pushed toward the loop?
Counterclockwise emf and current
Changing B
N
S
PHY2049: Chapter 30 8
B field points into screen. Is induced emfclockwise or couterclockwise?
Changing Area
v
PHY2049: Chapter 30 9
Another Example
What is the direction of induced emf?(a) Clockwise(b) Counterclockwise(c) No emf
I
pullRHR #2
RHR #3 and Lenz
PHY2049: Chapter 30 10
Current i due to emf receives force from B
Force required to pull the loop
Power (work per time) required to pull the loop
Power dissipated in the wire as heat
iLBF =
iLBF =req
Motional emf and Energy
Agrees!
LvBε =||
Ri ε ||=
( )( )
( )RLvBvF
FP
2
reqreq
req timedistance
===
( )RLvBR
RLvBRiP
222
diss =
==
F
i
i
PHY2049: Chapter 30 11
Electric Power Generation… when Faraday was endeavouring to explain to Gladstone (Chancellor of the Exchequer) and several others an important new discovery in science, Gladstone's only commentary was “but, after all, what use is it?” “Why, sir,” replied Faraday, “there is every probability that you will soon be able to tax it!”
W. E. H. Lecky, Democracy and Liberty (Longmans Green, London, 1899)