Maxwell’s equations

Maxwell’s equations are:

(SI units) (Gaussian units)
or, in macroscopic form:
In lih materials with

we have:

Maxwell’s equations are linear equations and the principle of superposition holds.

,

(SI units) (Gaussian units)

Faraday’s law

(SI units) Gaussian units)
Define the flux

and the electromotive force
.
Then :

Any induced emf tries to oppose the flux changes that produces it.  This is Lenz’s rule.

Quasi-static situations

Consider N  filamentary circuits.  Then the flux through the ith circuit is   where    (SI units),   (Gaussian units).

is the coefficient of mutual induction and   is the coefficient of self inductance.  We have

.

For a single filamentary circuit we have   . To change the current in a circuit we need an external emf, Vext, to overcome the induced emf e.

The energy stored in the circuit is .  For a system of N circuits we have:

(SI units) (Gaussian units)
or
or

Energy and momentum in electrodynamics

Poynting’s theorem,     is a statement of energy conservation.

(SI units),   (Gaussian units)

is the energy density and

(SI units),                     (Gaussian units)

is the energy flux in the electromagnetic field.  We define the momentum density as

(in SI and Gaussian units).

The Lorentz gauge

If in electrodynamics we choose the Lorentz gauge defined through

(SI units) (Gaussian units)
then f and each Cartesian component of A
satisfy the inhomogeneous wave equation
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Choosing     is called choosing the Coulomb gauge.