Wave propagation - Oblique Incidence

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SUMMARY

The discussion focuses on the analysis of a plane wave incident on a dielectric surface, specifically addressing the polarization, angle of incidence, and the derivation of time-domain expressions for the transmitted electric and magnetic fields. The incident wave is represented by the equation 𝐄̃i = 𝐲̂20𝑒−𝑗(3𝑥+4𝑧) [V. m−1], with the dielectric material characterized by εr = 4. The angle of incidence is determined using the tangent function, specifically tan(3/4), after establishing a new coordinate system to visualize the propagation direction.

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Ian751
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Misplaced Homework Thread: moved from technical forums so no template
Summary:: A plane wave incident upon a planar surface - determining polarization, angle of incidence etc.

𝐄̃i = 𝐲̂20𝑒−𝑗(3𝑥+4𝑧) [V. m−1 ]

is incident upon the planar surface of a dielectric material, with εr = 4, occupying the halfspace z ≥ 0.
a) What is the polarisation of the incident wave?
b) What is the angle of incidence?
c) Obtain time-domain expressions for the transmitted electric and magnetic fields.

I'm not too great with EM theory and am trying to improve here. Confused with how the angle of incidence is determined here and how to visualize it. I think I recognize the plane of incidence as the xy plane thus the electric field is perpendicularly polarized. If the direction of propagation is now determined by 3x + 4z, would it be correct to determine the angle of incidence by taking tan(3/4)?
 
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If I said 'yes' or 'no' that would not help you.
Suggestion:
rotate the x' axis by ## \theta ## wrt the x-axis about the y axis
define new axes x' = 3x + 4z, y' = y, z'

Then the direction of propagation is obviously in the x' direction.

Express x' in terms of ## \theta ## , x and z
From this you can compute ## \theta ##
 
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