51 ch29 induction

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Induction experiments (sec. 29.1) Faraday’s law (sec. 29.2) Lenz’s law (sec. 29.3) Motional electromotive force (sec. 29.4) Induced electric fields (sec. 29.5) Eddy currents (sec. 29.6) Displacement Current (sec. 29.7) Electromagnetic Induction Ch. 29 C 2012 J. F. Becker

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Induction

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AC CircuitsEddy currents (sec. 29.6)
Displacement Current (sec. 29.7)
Electromagnetic Induction Ch. 29
OVERVIEW
Learning Goals - we will learn: ch 29
• The experimental evidence that a changing magnetic field induces an emf !
• How Faraday’s Law relates the induced emf in a loop to the change in magnetic flux through the loop.
• How a changing magnetic flux generates an electric field that is very different from that produced by an arrangement of charges.
• Four fundamental equations completely describe both electricity and magnetism.
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When B is constant and the shape, location, and orientation of the coil does not change, the induced current is zero
in the coil.
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Lenz’s law
Lenz’s Law
The induced emf (or current) always tends to oppose or cancel the change that caused it.
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How electric generators, credit card readers, and transformers work.
A changing magnetic flux causes (induces) an emf in a conducting loop.
C 2004 Pearson Education / Addison Wesley
Eqn 29.3
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Lenz’s law
Lenz’s Law
The induced emf (or current) always tends to oppose or cancel the change that caused it.
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e = DV = energy / charge = W/q
e = DV = work / charge
DV = (q v B) L / q
so
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A capacitor being charged by a current iC has a “displacement current” between the plates equal to iC , with displacement current iD = e A dE/dt. This changing E field can be regarded as the source of the magnetic field between the plates. ( E _ B )
DISPLACEMENT
CURRENT
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A capacitor being charged by a current iC has a displacement current equal to iC between the plates, with
displacement current iD = e A dE/dt
From C = e A / d and DV = E d we can use
q = C V to get
q = (e A / d ) (E d ) = e E A = e F E and
from iC = dq / dt = e A dE / dt = e dF E / dt = iD
We now see that a
changing E field can produce a B field,
and from Faraday’s Law, a
changing B field can produce an E field or emf.
C 2011 J. Becker
C 2004 Pearson Educational / Addison Wesley
The relationships between electric and magnetic fields and their sources can be stated compactly in four equations, called
Maxwell’s equations.
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Lenz’s law
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Direction of induced current through R = ? when switch is closed, opened, coils are moved closer, R is decreased?
Lenz’s law (Exercise 29.18)
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Direction of induced current through R when current goes into, out of terminal a, input current is increasing or decreasing?
Motional emf and Lenz’s law
(Exercise 29.21)
(Exercise 29.26)
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Determine induced current directions as loop passes into, through, and out of B field.
TRANSFORMERS
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Direction of induced current through R when current goes into, out of terminal a, input current is increasing or decreasing?
Transformer: AC source is V1 and secondary provides a voltage V2 to a device with resistance R.
TRANSFORMERS
e2 /e1 = N2/N1
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Figure 32.2b
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OVERVIEW