Physics for Scientists and Engineers: A Strategic Approach with Modern Physics (4th Edition)

Published by Pearson
ISBN 10: 0133942651
ISBN 13: 978-0-13394-265-1

Chapter 34 - Ray Optics - Exercises and Problems - Page 990: 16

Answer

$d = \frac{R}{n}$

Work Step by Step

The light ray will travel straight into the transparent material. Then it will refract out through the curved surface as long as the angle does not exceed the critical angle. We can find the critical angle: $\theta_c = sin^{-1}~(\frac{n_2}{n_1})$ $\theta_c = sin^{-1}~(\frac{1}{n})$ Note that $sin~\theta_c = \frac{1}{n}$ Using geometry, we can see that the angle between the normal and the light ray striking the curved surface has the following relationship: $sin~\theta = \frac{d}{R}$ To find the maximum value of $d$, we can set this angle $\theta$ equal to $\theta_c$: $sin~\theta = \frac{d}{R}$ $sin~\theta_c = \frac{d}{R}$ $\frac{1}{n} = \frac{d}{R}$ $d = \frac{R}{n}$
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