Path of Light Beam in Plane Parallel Plate

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Homework Help Overview

The problem involves the path of a light beam in a plane parallel plate where the refractive index varies with the coordinate z, defined by the equation ##n=n_0 -{n}'z^2##. The task is to analyze this scenario under the paraxial approximation.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the implications of the varying refractive index and the use of parametrization in the context of the problem. There is an exploration of the relationship between the differentials ##dz## and ##dx##, with some questioning the appropriateness of the approximations used. Others consider the physical interpretation of the components derived from the vector equation.

Discussion Status

The discussion is ongoing, with participants clarifying their understanding of the paraxial approximation and its implications for the problem setup. Some guidance has been offered regarding the need to consider the components of the vector equation, and there is acknowledgment of confusion around the approximations used.

Contextual Notes

Participants note that the problem specifies the ray travels close to the center of the layer, where z is small, which influences the assumptions made about the relationships between differentials.

skrat
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Homework Statement


In plane parallel plate the refractive index is a function of coordinate ##z##, so that ##n=n_0 -{n}'z^2## for ##{n}'>0##. The origin of the coordinate system is in the middle of the layer, and ##z## is parallel to the normal of the layer. In paraxial approximation calculate the path of a light beam.

Homework Equations


If we use parametrization ##s##:

##\frac{d}{ds}(n(z)\frac{d\vec r}{ds})=\nabla n##

The Attempt at a Solution


For ##z## coordinate: $$\frac{d}{ds}(n(z)\frac{d z}{ds})=\frac{dn}{dz}=-2{n}'z$$ $$\frac{d}{ds}([n_0-{n}'z^2]\frac{d z}{ds})=-2{n}'z$$ Now I hope I can use approximation that ##dz\sim dx## this would bring me to $$[n_0-{n}'z^2]\frac{d^2z}{dx^2}=-2{n}'z$$ and finally since ##z## is very small, than I can forget about ##z^2## term. $${z}''+\frac{2{n}'}{n_0}z=0$$ which brings me to my final solution $$z(x)=Asin(\sqrt{\frac{2{n}'}{n_0}}x)+Bcos(\sqrt{\frac{2{n}'}{n_0}}x)$$
Or is this completely wrong?
 
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skrat said:
Now I hope I can use approximation that ##dz\sim dx##
Reconsider this. Paraxial means that the ray always makes a small angle to the z-axis.

Homework Equations


If we use parametrization ##s##:

##\frac{d}{ds}(n(z)\frac{d\vec r}{ds})=\nabla n##

Note that this is a vector equation. So, you will need to think about its components.
 
Hmmm, ok firstly, let me apologize for a mistake in my first post. There should be ##ds\approx dx## and not ##dz\approx ds##.
But you got me a bit confused now. I think you are trying to say that I should use approximation where ##ds\approx dz## but... this is in contrary with the problem. The problem says that the ray is only traveling close to the centre of the layer (where ##z## is very small). Or...?

The other two components only give me $$n(z)\frac{dx}{ds}=n(z)\sin\vartheta _x=C_x$$ and $$n(z)=\sin\vartheta _y=C_y.$$ Do they have any physical interpretation?
 
OK, I guess I misinterpreted the question. Since they only mention a z-axis, I assumed that paraxial meant that the ray is traveling approximately in the z-direction as it passes through the plate. So, yes, I was thinking ds ≅ dz.

[EDIT: I agree with your solution.]
 
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