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Electrodynamics

Electrodynamics

Electrodynamics

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From vacuum to dielectric media<br />

If there are no free charges or currents, but 0 and 0 (yet constants)<br />

<br />

The ratio<br />

is the index of refraction<br />

dispersion equation<br />

phase velocity (propagation of the constant phase)<br />

group velocity (propagation of energy and infromation!)<br />

In this case the phase and group velocities are the same.<br />

We say that the medium is non-dispersive.<br />

It means that waves with all frequencies / wave numbers<br />

propagate with the same velocity<br />

If in addition J = E ( constant), the situation becomes more complicated<br />

<br />

One form of so-called telegrapher’s equations;<br />

a standard class-room example of using Fourier<br />

transformations to solve partial differential equations<br />

Instead of making the Fourier transformations, let’s start from Maxwell’s<br />

equations and make the plane wave assumption<br />

Clearly k, E and H are all perpendicular<br />

to each other: transverse wave<br />

Choose: k || e z , E || e x , H || e y<br />

<br />

<br />

dispersion equation<br />

now !<br />

8

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