Reflection and Refraction — Question 3

Section 33-7 · Physics pages 5496–5497

Question 3 A parallel slab shifts a ray without changing its final direction A plate of thickness d and refractive index n is surrounded by air. A ray enters at angle i from the normal, refracts to r, and exits the parallel rear face. Assume n greater than one. d Schematic; labels, not drawing lengths, specify the data. (a) Derive the exit angle and the perpendicular separation between the outgoing ray and the undeviated continuation of the incoming ray. (b) Find the small-incidence approximation to the displacement, with i in radians.
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Question 3 - Solution A parallel slab shifts a ray without changing its final direction d (a) Method and calculation sin i = n sin r, n sin r = sin iout ⇒iout = i . ∆x = d(tan i −tan r), D = ∆x cos i = d sin(i −r)/ cos r . (b) Interpretation and further calculation r ≃i/n, sin(i −r) ≃i(1 −1/n), cos r ≃1. D ≃di(1 −1/n) . Physical check The lateral separation D is measured perpendicular to the parallel external rays; it is not the displacement measured along the rear surface.

Question 3

A parallel slab shifts a ray without changing its final direction

A plate of thickness d and refractive index n is surrounded by air. A ray enters at angle i from the normal, refracts to r, and exits the parallel rear face. Assume n greater than one.

Diagram shown in the original SVG worksheet.

  1. Derive the exit angle and the perpendicular separation between the outgoing ray and the undeviated continuation of the incoming ray.

  2. Find the small-incidence approximation to the displacement, with i in radians.

Question 3 - Solution

A parallel slab shifts a ray without changing its final direction

Diagram shown in the original SVG worksheet.

(a) Method and calculation

sin⁡i=nsin⁡r,nsin⁡r=sin⁡iout⇒iout=i.\sin i=n\sin r,\quad n\sin r=\sin i_{\mathrm{out}}\Rightarrow\boxed{i_{\mathrm{out}}=i}.Δx=d(tan⁡i−tan⁡r),D=Δxcos⁡i=dsin⁡(i−r)/cos⁡r.\Delta x=d(\tan i-\tan r),\quad D=\Delta x\cos i=\boxed{d\sin(i-r)/\cos r}.

(b) Interpretation and further calculation

r≃i/n,sin⁡(i−r)≃i(1−1/n),cos⁡r≃1.r\simeq i/n,\quad\sin(i-r)\simeq i(1-1/n),\quad\cos r\simeq1.D≃di(1−1/n).\boxed{D\simeq di(1-1/n)}.

Physical check

The lateral separation D is measured perpendicular to the parallel external rays; it is not the displacement measured along the rear surface.