Deflection of wave in dissipative media with a complex refractive index

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Homework Help Overview

The problem involves a monochromatic plane wave with a wavelength of 500µm propagating through a dissipative medium characterized by a complex refractive index of 1-0.0002i. The wave is approaching the boundary of the medium and transitioning into free space, raising questions about the deflection of the wave as it exits the medium at an angle of incidence that is not 90°.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • The original poster attempts to apply Snell's Law but expresses uncertainty about finding the angles involved in the transition from the medium to free space. Some participants provide insights into the propagation of waves in media with complex refractive indices and discuss the factors influencing boundary conditions.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of the problem. Some guidance has been offered regarding the role of the real part of the refractive index in determining the direction of the wavefront at the boundary. However, there is acknowledgment of differing perspectives on the topic, indicating a lack of consensus on a definitive answer.

Contextual Notes

Participants note that the complexity of the refractive index may complicate experimental verification of results, particularly if the imaginary component becomes significant. There is also mention of various interpretations of the laws of refraction, suggesting that assumptions about the behavior of the wave may vary among sources.

Tinaaaaaa
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Homework Statement


A monochromatic plane wave with wavelength 500µm is propagating through a dissipative medium with refractive index 1-0.0002i. It approaching the edge of the medium, and will pass out into free space. If the angle of incidence is not 90°, how much will the wave deflect as it passes out into free space?

Homework Equations


Snell's Law:
b5a73124df21668801a4d20054bb1b13f6709752


The Attempt at a Solution


The refractive index of free space would be 1-0*i so so far I have 1-0.0002i/1. But I don't know how to find the angles.
 
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I haven't previously worked this type of problem, even though I have an Optics background, but I can give you a couple of inputs to it. In a medium with complex ## n ##, the wave will propagate as ## E=E_o e^{i( n_r k_o x-\omega t)} e^{-n_i k_o x} ##. I don't think the ## e^{-n_i k_o x } ## factor will affect the boundary value conditions that determine which direction the wavefront emerges when it encounters a boundary. I think that is simply determined by ## n_r ##. If my inputs are indeed correct, the answer to this problem, for which ## n_r=1 ##, should be obvious.
 
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Charles Link said:
I haven't previously worked this type of problem, even though I have an Optics background, but I can give you a couple of inputs to it. In a medium with complex ## n ##, the wave will propagate as ## E=E_o e^{i( n_r k_o x-\omega t)} e^{-n_i k_o x} ##. I don't think the ## e^{-n_i k_o x } ## factor will affect the boundary value conditions that determine which direction the wavefront emerges when it encounters a boundary. I think that is simply determined by ## n_r ##. If my inputs are indeed correct, the answer to this problem, for which ## n_r=1 ##, should be obvious.
Thank you this makes a lot of sense
 
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Tinaaaaaa said:
Thank you this makes a lot of sense
A google of this question shows there seems to be a couple of different schools of thought on the subject. There are a couple of postings that talk about the Descartes-Snell law of refraction, but there are other postings that interpret it exactly like I did. I leave the question open to further discussion, but I don't know that there is a definitive answer to this one that everyone will agree upon. ## \\ ## Unless ## n_i ## is considerably greater than ## 0 ##, it may be difficult to experimentally verify any result that would show ## n_i ## could cause some effect, but if ## n_i ## gets to be significant, the wave doesn't propagate very far through the material.
 

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