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Electromagnetic Waves

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Maxwell Equations<br />

⋆ A basic feature of Maxwell equations for the EM field is the existence<br />

of travelling wave solutions which represent the transport of energy from<br />

one point to another.<br />

⋆ The simplest and most fundamental EM waves are transverse, plane<br />

waves.<br />

In a region of space where there are no free sources (ρ = 0, J = 0),<br />

Maxwell’s equations reduce to a simple form given<br />

∇ · E = 0 , ∇ × E <br />

1 ∂<br />

+<br />

c<br />

B<br />

∂t<br />

∇ · B = 0 , ∇ × B − µɛ<br />

c<br />

where D and H are given by relations<br />

∂ E<br />

∂t<br />

= 0<br />

= 0 (1)<br />

D = ɛ E and H = 1<br />

µ B (2)<br />

where ɛ is the electric permittivity and µ the magnetic permeability<br />

which assumed to be independent of the frequency.<br />

<strong>Electromagnetic</strong> <strong>Waves</strong>

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