Maxwells equations
are:| (SI units) | (Gaussian units) | |
| or, in macroscopic form: | ||
| In lih materials with we have: |
||
Maxwells equations are linear equations and the principle of superposition holds.
,
| (SI units) | (Gaussian units) | |
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| (SI units) | Gaussian units) | |
| Define the flux and the electromotive force Then : |
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Any induced emf tries to oppose the flux changes that produces it. This is Lenzs rule.
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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 | |||
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Poyntings theorem
,
(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).
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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 |
||
Choosing
is called
choosing the Coulomb gauge.