Download Magnetic Flux Faraday`s Law

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Transcript
2/25/2014
Magnetic Flux
• Recall: when you put a loop of wire in
a magnetic field it will rotate until the
magnetic moment (the vector normal
to area) is aligned with the field.
• The degree of alignment with the field
is measured using magnetic flux Φ஻ :
Φ஻ ≡ ‫ ܣ ܤ‬cos ߠ
• Magnetic flux tells us how much field
is passing through the loop given the
angle between field and normal
• Magnetic flux is measured in Tmଶ
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Faraday’s Law
• Principle of EM induction: A change in the magnetic
flux through a loop produces an a induced ‘EMF’ or
electromotive force (voltage) ℰ and therefore an
induced current in the loop is given by Faraday’s Law:
∆Φ஻
ℰ = −ܰ
∆‫ݐ‬
• The minus sign tells us that the induced emf would be
created so that its own field points in a direction
opposite to the change in the field causing it in the first
place. (Lenz’s Law; coming up shortly)
• Simulation:
http://phet.colorado.edu/en/simulation/faraday
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2/25/2014
Example
• For a coil with ܰ = 2, ‫ = ܣ‬0.0050 mଶ , ‫ ܤ‬௜ =
0.010 T, ߠ = 0°, the field changes to ‫ ܤ‬௙ =
0.030 T still in the same direction. What’s the
resulting emf ℰ if the change took one
∆஍
second? ℰ = −ܰ ∆௧ಳ
∆Φ஻ = Φ௙ − Φ௜
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Lenz’s Law
• Lenz’s Law: The direction
of the induced emf and
induced current will be
such as to produce a
magnetic field which
opposes the original
change in magnetic flux
• This is needed to prevent a
violation of the
conservation of energy!
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2/25/2014
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Examples
10
Applications: 1. Induction Motor
• As the coil is rotated in
the magnetic field flux
changes and induces
current to flow in the coil
• What is the direction of
the current in the coil?
11
Applications: 2. Magnetic Induction
Stoves
• Magnetic induction
cooking.
• The magnetic field
induces an electric field in
the metal of the pan.
• never use aluminum foil
on it!
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2/25/2014
Electrical Resistance
• We have already seen in lab that
current and potential difference
(voltage) are related through Ohm’s
Law:
∆ܸ
‫=ܫ‬
ܴ
• where ܴ is the resistance measured in
ohms Ω = V/A
• Since emf (ℰ) is a potential difference,
for a coil where flux is changing we
have:
ℰ
ܰ ∆Φ஻
‫ܫ‬௜௡ௗ௨௖௘ௗ = = −
ܴ
ܴ ∆‫ݐ‬
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