Electromagnetic induction
§ 1 The phenomenon of electromagnetic induction.
Faraday's law
 Faraday's experiments
a) The
solenoid, closed the galvanometer, pushed into and put forward the
permanent magnet. The galvanometer deflection will, and it will be
longer than the faster the pushed into and put forward. When you change
the direction of the poles of the magnet deflection change.
b)
solenoid, closed the galvanometer is inserted coil (another solenoid)
through which current is passed. When you turn on and off (ie, any
change in the current) is deflection of the galvanometer. Direction of
the deviation varies with On  Off, decrease  the current increases,
vdviganii  sliding out the coils.
The
phenomenon of electromagnetic induction is that in a closed conducting
circuit when the flow of magnetic induction covered by this contour,
an induction (induced) electric current.
Occurrence of the induced current means that the circuit operates electromotive force E_{i}  induced emf.
EMF
induction, which occurs in the conducting circuit, equal to the rate
of change of magnetic flux through the area bounded by this contour 
Faraday's law.
In 1834, E.H. Lenz established the law, allowing to determine the direction of induced current.
Lenz rule: induction loop current always has a direction such that
the magnetic field created by it prevents the change in magnetic flux
that caused this induced current.
The minus sign in Faraday's Law is a mathematical expression of the rule of Lenz.
If the circuit in which the induced emf is not composed of a single
turn, and of N turns (eg, solenoid), if windings are connected in
series, E_{i} will be equal to the emf induced in each of the coils individually:
flux linkage or the total magnetic flux.
If Ф_{1} =Ф_{2}=…=Ф_{n}, then
Because Ф_{B}=BScosα, then in order to change the magnetic flux F can be changed:
1)magnetic field ;
2) the area S;
3) the angle α.
§2 Spin current loop in a magnetic field
The phenomenon of
electromagnetic induction is used to convert mechanical energy and the
energy of the electric current in the generator current loop area S
rotates in a uniform magnetic field ()evenly with a constant angular velocity ω.
α = ωt.
Then
At sin ωt=1
and
Because network frequency , then for increase
need to increase
B and S. As can be increased by using powerful permanent magnets or
electromagnets to pass large currents. Core with a large electromagnet
choose μ. To increase the use of S multiturn coil.
If a current loop placed in a magnetic field, an electric current, then it will be acted torque
and the current loop starts to rotate. Based on this principle of the motor, designed to transform electrical energy into mechanical energy.
§3 Foucault currents.
Induced currents can be excited in continuous bulk conductors. In this
case they are called Foucault currents or eddy currents. The
electrical resistance of a bulk conductor is small, so eddy currents
can reach a very large force.
Eddy currents,
as well as induced currents in linear conductors are subject Lenz's
law: their magnetic field is directed so to counteract changes in the
magnetic field that induces eddy currents.
Therefore,
moving in a strong magnetic field are good conductors under heavy
braking due to the interaction of the eddy currents and the magnetic
field. It is used for damping (steadying) of moving parts
galvanometers, seismographs, etc. Thermal effect of the eddy currents is
used in induction melting furnaces.
To reduce eddy currents transformer cores made ??of individual plates and the plates are perpendicular to the currents of Foucault.
S due to
eddy currents rapidly current unevenly distributed over the cross
section of wire  it pushed to the surface of a conductor  the skin
effect. Therefore, at high frequencies using hollow wire.
§ 4 of the circuit inductance.
Selfinduction
In
any case where the contour of the electric current creates a magnetic
field. In this case, there is always a magnetic flux F passing through
the surface bounded by the circuit under consideration. Any change in
the current in the circuit changes the magnetic field, coupled with the
circuit, and this in turn causes the induced current. This phenomenon
is called selfinduction: the emergence of the emf induced in a
conductor when the current in it.
Of the BiotSavartLaplace should
ie magnetic flux linked with the circuit is proportional to the current I in the circuit
Ф=LI.
[L] = H (henry).
1 H  inductance of the loop, the magnetic flux is selfinduced by a current of 1 A is 1 Wb
.
Calculate the inductance L of the solenoid
magnetic induction of the solenoid
ie inductance depends on the geometry of the solenoid (),number of turns and
the magnetic permeability of the core solenoid. Therefore we can say
that the inductance L capacitance C analogue isolated conductor, which
also depends on the geometry, the shape and the dielectric constant of
the medium.
Applying the selfinduction Faraday's law, we find that selfinduced emf
If L = const
where the minus sign, due to Lenz's law, shows that the presence of inductance in the circuit slows current change in him.
If the current increases with time , then , and ie current is directed towards the selfinductance of the current, due to the external source and inhibits its growth. If the current time is decreasing, then and ie
induced current has the same direction as the decreasing current in
the circuit, and slows its decay. Consequently, the circuit having
inductance is electrically inert, consists in the fact that any change
in the current is inhibited, the stronger, the more inductance.
