Planar wave normally incident on dielectric boundary

[cfitzU2]

PROBLEM: I am asked to consider a parallel polarized planar wave with frequency ω is normally incident on a dielectric boundary. The incident time average power flux P_i = 100 w/m^2. The first medium is free space and the second has vacuum permeability but ε=4ε_0. We are also given that the medium is characterized by conductivity σ.

I am then asked to find the reflected time average power flux P_reflected in two cases

(i) σ/(ω*ε_0)<<1 and (ii) σ/(ω*ε_0)>>1


My problem is that, while performing the calculation I see no use for the quantity in question, namely, σ/(ω*ε_0)...


ATTEMPT: I am able to find the reflected time average power flux using P_i = (1/2*η)(E_i)^2 = 100 w/m^2 with P_reflected = (1/2*η)(E_r)^2 and E_r = ρE_i where ρ=(η_2 - η)/(η+η_2).

This is especially simple after noting that η_2 = (1/2)η

The calculation leads to P_reflected = 100/9 w/m^2

I see no opportunity to consider how varying the conductivity changes that number... I realize that as σ gets big η_2 must go to zero... but we are given a fixed ε=4*ε_0

Am I missing something or is this a poorly posed (or trick) problem??

 

[note360]

Note that the permitivity can me complex, but only the real part has been given. Remember that \eta is described interms of: \eta = \sqrt{\frac{\mu_0}{\textbf{ε}}}, where \epsilon is actually the complex permitivity.

There is plenty potential to use \frac{\sigma}{\omega * \epsilon_{0}} &lt;&lt; 1 and \frac{\sigma}{\omega * \epsilon_{0}} &gt;&gt; 1 cases