rotating the magnet changes the angle between the coil and B
Magnetic Flux
Number of field lines passing through loop
size of magnetic field
area of loop
angle loop makes with field
B = magnetic field (uniform)
A = area of loop
q = angle between B and the normal to the loop
general expression if the field is not uniform.
magnetic flux has units of [T-m2] = [Weber]
Faraday's Law
Induced emf
depends on rate of change of magnetic flux
one loop
N loops
Use Faraday's Law to get magnitude of the induced voltage
Lenz's Law
The direction of the induced emf is such that it will oppose the change
that created it.
Lenz's Law will give the direction or polarity of the emf.
Examples
Motional Emf
conducting rod moving through a magnetic field
charges can move freely in the rod.
with the rod moving as shown through a
magnetic field pointing into the page,
positive charges will migrate to the top
end of the rod and negative charges will
migrate to the bottom end of the rod.
this will continue until the electric force balances the magnetic
force.
if we put this rod on conducting rails and connect a load to complete
the circuit
then
we can use Faraday's Law to determine the induced emf
for the loop.
Lenz's Law
flux is increasing downward, induced current must produce
magnetic field pointing out of page
current will be in CCW matching the polarity found using the
motional emf approach.
Examples
Inductors
consider a very simple circuit consisting of a battery, resistor and a
switch.
When the circuit is closed, current will flow. This
produces a changing magnetic flux inside the loop of
the circuit. This will induce an emf directed such that it
opposes the change in current.
With an inductor added to the circuit, we have the
circuit shown. Applying the loop rule gives
The solution to this equation is
The inductor will also play a role when the switch is opened and the
current is decreasing.
Energy Stored in a Magnetic Field
applying the loop rule again and multiplying the equation by I
IV represents the rate at which energy is being
provided to the
circuit by the battery.
not all of that energy is being dissipated in the resistor, some
of it is going to the inductor.
the inductor is storing energy similar to the capacitor in
an RC circuit.
when the switch is opened, the inductor will induce an emf that
will try to keep current moving. After the switch is opened, the
resistor will dissipate the energy stored in the inductor.