Now we will take a look at wave propagation in homogeneous, lossless,^{14} non-conducting media. Again we start with Maxwell's first and second equation in differential form

We are interested in non-conducting media so the conductivity is zero (σ = 0) and there is no conduction current density . On the right-hand side of Ampere's law (Equation 2.88) only the displacement current density remains. First we apply the curl operator and the constitutive relation (with μ = μ_{0}μ_{r}) on Equation 2.89.

Now we insert Equation 2.88 into Equation 2.90 by using the constitutive relation (with ε = ε_{0}ε_{r}). Since we assume the medium to be time-invariant we can write the material parameters outside the derivative.

2.91

As in our discussion ...

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