Change of phase in total internal reflection

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Discussion Overview

The discussion centers on the phase change during total internal reflection, particularly in the context of a thin glass layer over copper and its interaction with electromagnetic waves at 200 MHz. Participants explore the implications of the layer's thickness and material properties on reflection and phase behavior.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant inquires about the phase change during total internal reflection, specifically with a glass layer over copper reflecting 200 MHz EM waves from water.
  • Another participant suggests that the thin glass layer would not significantly affect the reflection, as the copper would dominate due to its reflective properties.
  • Concerns are raised about the phase change associated with the thin copper layer, which reflects nearly all wave energy, prompting interest in the phase change at the water/glass interface.
  • Some participants argue that the thinness of the glass layer means it cannot significantly alter the phase, with transit times being very short.
  • Discussion includes the concept of skin depth in copper and how it differs from the behavior of glass as a dielectric, affecting wave penetration and evanescent wave formation.
  • Questions arise regarding the phase behavior during total internal reflection when a thick enough dielectric layer is present.
  • Mathematical expressions for the reflection coefficient are provided, indicating that for a thin dielectric, the reflection coefficient approaches -1, suggesting minimal impact from the dielectric layer.
  • One participant calculates the total reflection coefficient for a specific scenario involving a water interface over copper, expressing it in complex form.
  • Clarification is sought regarding the notation used in the complex reflection coefficient calculation.

Areas of Agreement / Disagreement

Participants express differing views on the impact of the thin glass layer on phase change and reflection properties. The discussion remains unresolved regarding the exact effects of the dielectric layer and the implications for phase behavior during total internal reflection.

Contextual Notes

Limitations include assumptions about the thickness of layers, the dependence on material properties, and the specific conditions under which the phase change is evaluated. The discussion does not resolve the mathematical complexities involved in the reflection coefficient calculations.

htg
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I would like to know if there is change of phase during total internal reflection. (In particular I would like to know if I can cover copper with several microns of glass and have it reflect 200 MHz EM waves coming from water (epsilon(H2O)=80, epsilon(glass)=4)).
 
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The thin layer (compared with the wavelength involved) of glass would not have any significant effect, I think. The copper would dominate and it would be a case of reflection by a metal surface.
 
It it not clear to me. The layer of copper is also thin, but it reflects close to 100% of tha wave energy. This is why I am interested in the phase change in the case of reflection from the water/glass interface.
 
But it can't significantly alter the phase as its so thin - the transit time must be only a few picoseconds.
 
sophiecentaur said:
But it can't significantly alter the phase as its so thin - the transit time must be only a few picoseconds.
Somehow comparably thin layer of Cu changes the phase by about Pi radians during reflection.
 
Ah yes but the skin depth is minute for copper because of it high conductivity. Glass is a dielectric and things are different because the wave can penetrate. The evanescent wave 'behind' the interface doesn't have a chance to form before it hits the copper.
 
sophiecentaur said:
Ah yes but the skin depth is minute for copper because of it high conductivity. Glass is a dielectric and things are different because the wave can penetrate. The evanescent wave 'behind' the interface doesn't have a chance to form before it hits the copper.
I hope you are right. By the way, what happens to phase during total internal reflection when we have a thick enough layer of dielectric?
 
200 MHz corresponds still to a wavelength on the order of 1 meter in glass.
To see an effect of the glass on the radio waves it should be at least as thick.
In copper the situation is different. The dielectric constant is very large and negative so that the penetration depth is only, say, some micro meters.
 
htg said:
I hope you are right. By the way, what happens to phase during total internal reflection when we have a thick enough layer of dielectric?

As I recall, the reflection coefficient is +1 for total internal reflection at a dielectric to dielectric interface at the critical angle. But of course there is a 180 degree phase shift for one of the components (the magnetic field I think) due to the change in the direction. Beyond the critical angle, the reflection coefficient becomes complex and you introduce a phase shift to both components I believe.

But yeah, having a thin layer of dielectric on the copper is not going to do anything. The resulting reflection coefficient is

R = \frac{R_{12}+R_{23}e^{2ik_zd}}{1+R_{12}R_{23}e^{2ik_zd}}

For a thin dielectric the exponential is approximately 1 and R_{23} = -1 for a PEC and thus the total reflection coefficient is approximately -1. So no real difference.

We can also recast it as

R = R_{12} + \frac{T_{12}R_{23}T_{21}e^{2ik_zd}}{1-R_{21}R_{23}e^{2ik_zd}}

If we have total internal reflection, then R_{21} = 1, T_{21} = 2 and as before R_{23} = -1. Thus,

R = R_{12} - T_{12} = -1

We can easily calculate this exactly for a water interface of 1 mm over copper with an incident angle of 45 degrees. The total reflection coefficient is -1 - 2.40081795943819e-009i.
 
Last edited:
  • #10
Born2bwire said:
We can easily calculate this exactly for a water interface of 1 mm over copper with an incident angle of 45 degrees.
The total reflection coefficient is -1 - 2.40081795943819e-009i.

What is e-009i ? (The decimal point of the exponent is not there)
 
  • #11
htg said:
What is e-009i ? (The decimal point of the exponent is not there)

10^(-9)*i.
 

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