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The relationship between changing magnetic fields, magnetic flux, and the induced electric fields through various examples and formulas. Topics include faraday's law, lenz's law, and the calculation of magnetic flux through different shapes. The document also covers the concepts of conservative and nonconservative electric fields, and the phenomenon of diamagnetism.
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It takes fourteen 110-car trainloads of each week to fuel this power plant.What feature of the equation
ε^
=^
-
d Φ
/ B dt
demands this prodigious fuel consumption?
The minus sign, which denotes energy conservation in electromagnetic induction.
changing
induces currents (electromagnetic induction)
-^
A solenoid of circular cross section has radius
consists of
n
turns per unit length, and carries current
Find the magnetic flux through each turn of the solenoid.
2
0
n I
B^
out of plane
A long, straight wire carries current
A rectangular wire loop of dimensions
l^
by
w
lies in a plane containing
the wire, with its closest edge a distance
a
from the wire, and its
dimension
l^
parallel to the wire.
Find the magnetic flux through the loop.
0 2 a^
w a
l dr r
B^
d
^
a^
w a
I l
d r r
0
ln
I l
a^
w a
Area element for integration
A wire loop of radius 10 cm has resistance 2.
.
The plane of the loop is perpendicular to a uniform
B
that’s increasing at 0.10 T/s.
Find the magnitude of the induced current in the loop.
2
r
B^
B
d
d^
r
d t
d t
3
2
d B r^
d t
B
d d t
2
m
s
3
3
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A wire loop of radius 10 cm has resistance 2.
.
The plane of the loop is perpendicular to a uniform
B
that’s increasing at 0.10 T/s.
Find the magnitude of the induced current in the loop.
2
r
B^
B
d^
d
r
d t
d t
3
2
d B r^
d t
B
d d t
2
m
s
3
3
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Two parallel conducting rails a distance
l^
apart are connected at one end by a resistance
R
.
A conducting bar completes the circuit, joining the two rails electrically but free to slide along.The whole circuit is perpendicular to a uniform
B
, as show in figure.
Find the current when the bar is pulled to the right with constant speed
v
.
l x
B^
B
d
d t
Let E
x
= 0 be at the left end of rail.
l v
B l v
x
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Direction of emf is to opposemagnet’s motion.
Lenz’s law :Direction of induced emf issuch that
created by the
induced current opposes thechanges in
that created
the current.
Magnet moving right
RH rule: thumb //
m
.
Loop ~ magnet with N to left.^ RH rule: thumb //
m
.
Loop ~ magnet with S to left.
Magnet moving left
m
I I
m
Motional emf: induced emf due tomotion of conductor in
Square loop of sides
& resistance
pulled with
constant speed
v
out of uniform
Force on
e
v^
downward force
upward
Force on current carrying wire:
mag
, mag net
applied
B^
B L x
d^
B L v
d t
x^
B L v E P
B L v
B L v
F v
F v
I L B v
B L v
Work done is used to heat up circuit ( E conservation ).
d x
v
d t
CW
B
d
d t
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What will be the direction of the current when the loop firstenters the field from the left side?
Current is CCW
B
d
d t
B
d
d t
B
What will be the direction of the current when the loop firstenters the field from the left side?
Current is CCW
B
d
d t
B
d
d t
B