Electro-Motive Force: Electro-motive force is a generalisation
of the idea of electric potential to non-conservative electric fields.
The electromotive force in a circuit Γ is defined
to be
.
The EMF is measured in volts and it plays the same role in Ohm's Law that
the electrostatic potential did. Thus an EMF V will cause a current
to flow in a resistance R.
Faraday's Law: When the magnetic flux through a closed circuit
Γ changes, an EMF is introduced in the circuit
according to the equation
where S is any surface bounded by Γ.
Lenz's Law: The induced current acts to oppose the change that caused it. That is, the current flows in such a direction as to create a magnetic field that treis to keep the total flux constant.
Faraday's Law in differential form: application of Stoke's Theorem
to Faraday's Law gives a differential form of the law
.
A magnetic field B stores energy. The energy density (energy per unit
volume) stored in a field of intensity B is
.
Self-Inductance: Faraday's Law causes a coil that carries a changing
current I to create an induced EMF that opposes changes in the current.
The induced EMF is given by
where
L is a constant that describes the geometry of the coil. It is called
the Self Inductance of the coil and is measured in units of Henries.
For a given coil geometry the inductance L can be calculated by computing
the total magnetic flux, ΦM, that
is created in the coil by a current I and using
.
For example, a long solenoid of length l (that is a letter el), radius
R, wound with N turns of wire has an inductance
.
If two coils are placed so that flux from one coil passes through the
other coil then a changing current I1 in the first coil will
induce an EMF V2 in the second coil where
.
The constant M is called the Mutual Inductance and it depends only
on the geometry of the two coils.