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Planar wave normally incident on dielectric boundary

  1. Oct 15, 2012 #1
    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 vaccum 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??
     
  2. jcsd
  3. Oct 18, 2012 #2
    Note that the permitivity can me complex, but only the real part has been given. Remember that [itex]\eta[/itex] is described interms of: [itex]\eta = \sqrt{\frac{\mu_0}{\textbf{ε}}}[/itex], where [itex]\epsilon[/itex] is actually the complex permitivity.

    There is plenty potential to use [itex] \frac{\sigma}{\omega * \epsilon_{0}} << 1[/itex] and [itex] \frac{\sigma}{\omega * \epsilon_{0}} >> 1[/itex] cases
     
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