- #1
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?