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Transcript
Electromagnetic Induction
Michael Faraday





1791 – 1867
Great experimental
scientist
Invented electric
motor, generator
and transformers
Discovered
electromagnetic
induction
Discovered laws of
electrolysis
Faraday’s Experiment –
Set Up

A current can be produced by a
changing magnetic field

First shown in an experiment by Michael
Faraday


A primary coil is connected to a battery
A secondary coil is connected to an ammeter
Faraday’s Experiment




The purpose of the secondary circuit is to
detect current that might be produced by
the magnetic field
When the switch is closed, the ammeter
reads a current and then returns to zero
When the switch is opened, the ammeter
reads a current in the opposite direction
and then returns to zero
When there is a steady current in the
primary circuit, the ammeter reads zero
Faraday’s Conclusions



An electrical current is produced by a
changing magnetic field
The secondary circuit acts as if a source
of emf were connected to it for a short
time
It is customary to say that an induced
emf is produced in the secondary circuit
by the changing magnetic field
Magnetic Flux



The emf is actually induced by a change
in the quantity called the magnetic flux
rather than simply by a change in the
magnetic field
Magnetic flux is defined in a manner
similar to that of electrical flux
Magnetic flux is proportional to both the
strength of the magnetic field passing
through the plane of a loop of wire and
the area of the loop
Magnetic Flux


When the field is perpendicular to the plane of
the loop, as in a, θ = 0 and ΦB = ΦB, max = BA
When the field is parallel to the plane of the
loop, as in b, θ = 90° and ΦB = 0


The flux can be negative, for example if θ = 180°
SI units of flux are T. m² = Wb (Weber)
Magnetic Flux, final

The flux can be visualized with respect
to magnetic field lines



The value of the magnetic flux is
proportional to the total number of
lines passing through the loop
When the area is perpendicular to the
lines, the maximum number of lines
pass through the area and the flux is a
maximum
When the area is parallel to the lines,
no lines pass through the area and the
flux is 0
Electromagnetic Induction –
An Experiment




When a magnet moves
toward a loop of wire, the
ammeter shows the
presence of a current (a)
When the magnet is held
stationary, there is no
current (b)
When the magnet moves
away from the loop, the
ammeter shows a current
in the opposite direction (c)
If the loop is moved instead
of the magnet, a current is
also detected
Electromagnetic Induction –
Results of the Experiment

A current is set up in the circuit as
long as there is relative motion
between the magnet and the loop


The same experimental results are
found whether the loop moves or the
magnet moves
The current is called an induced
current because is it produced by
an induced emf
Faraday’s Law and
Electromagnetic Induction


The instantaneous emf induced in a
circuit equals the time rate of change
of magnetic flux through the circuit
If a circuit contains N tightly wound
loops and the flux changes by ΔΦB
during a time interval Δt, the
average emf induced is given by
Faraday’s Law:

  N
B
t
Motional emf


A straight conductor of
length ℓ moves
perpendicularly with
constant velocity
through a uniform field
The electrons in the
conductor experience a
magnetic force


F=qvB
The electrons tend to
move to the lower end
of the conductor
Motional emf



As the negative charges accumulate at the
base, a net positive charge exists at the
upper end of the conductor
As a result of this charge separation, an
electric field is produced in the conductor
The potential difference between the
ends of the conductor can be found by


ΔV = B ℓ v
The upper end is at a higher potential than
the lower end
Generators

Alternating Current (AC) generator



Converts mechanical energy to electrical
energy
Consists of a wire loop rotated by some
external means
There are a variety of sources that can
supply the energy to rotate the loop

These may include falling water, heat by burning
coal to produce steam
AC Generators, cont

Basic operation of the
generator




As the loop rotates, the
magnetic flux through it
changes with time
This induces an emf and a
current in the external circuit
The ends of the loop are
connected to slip rings that
rotate with the loop
Connections to the external
circuit are made by stationary
brushes in contact with the
slip rings
AC Generators, final

If the loop rotates with a
constant angular speed,
ω, and N turns
ε=NBAω
DC Generators


Components are
essentially the same
as that of an ac
generator
The major difference
is the contacts to the
rotating loop are
made by a split ring,
or commutator
DC Generators, cont



The output voltage
always has the same
polarity
The current is a
pulsing current
To produce a steady
current, many loops
and commutators
around the axis of
rotation are used

The multiple outputs
are superimposed and
the output is almost
free of fluctuations
Motors

Motors are devices that convert
electrical energy into mechanical
energy


A motor is a generator run in reverse
A motor can perform useful
mechanical work when a shaft
connected to its rotating coil is
attached to some external device
Nikola Tesla



1865 – 1943
Inventor
Key figure in
development of



AC electricity
High-voltage
transformers
Transport of electrical
power via AC
transmission lines

Beat Edison’s idea of
DC transmission lines
Transformers and Transmission of Power
A transformer consists of two coils, either interwoven or
linked by an iron core. A changing emf in one induces an
emf in the other.
The ratio of the emfs is equal to the ratio of the number
of turns in each coil:
Transformers and Transmission of Power
This is a step-up
transformer – the emf in the
secondary coil is larger than
the emf in the primary:
Transformers and Transmission of Power
Energy must be conserved; therefore, in the absence of
losses, the ratio of the currents must be the inverse of the
ratio of turns:
Electrical Power
Transmission

When transmitting electric power over
long distances, it is most economical to
use high voltage and low current


Minimizes I2R power losses
In practice, voltage is stepped up to
about 230 000 V at the generating
station and stepped down to 20 000 V
at the distribution station and finally to
120 V at the customer’s utility pole
Transformers and Transmission of
Power
Transformers work only if the current is changing; this is
one reason why electricity is transmitted as ac.