Fundamentals of Physics Extended (10th Edition)

Published by Wiley
ISBN 10: 1-11823-072-8
ISBN 13: 978-1-11823-072-5

Chapter 33 - Electromagnetic Waves - Problems - Page 1005: 63a

Answer

The index of refraction of the prism is $~~\sqrt{1.00+sin^2~\theta}$

Work Step by Step

Let $\theta_2$ be the angle of refraction when the ray enters the prism. Let $n_p$ be the index of refraction for the prism. We can use Snell's law to find an equation: $n_p~sin~\theta_2 = n_1~sin~\theta$ $n_p~sin~\theta_2 = 1.00~sin~\theta$ $n_p^2~sin^2~\theta_2 = sin^2~\theta$ Then the incident angle as the ray leaves the prism is $~~90^{\circ}-\theta_2$ We can use Snell's law to find an equation: $n_p~sin~(90^{\circ}-\theta_2) = n_1~sin~90^{\circ}$ $n_p~cos~\theta_2 = 1.00$ $n_p^2~cos^2~\theta_2 = 1.00$ We can add both sides of both equations: $n_p^2~sin^2~\theta_2+n_p^2~cos^2~\theta_2 = 1.00+sin^2~\theta$ $n_p^2~(sin^2~\theta_2+cos^2~\theta_2) = 1.00+sin^2~\theta$ $n_p^2 = 1.00+sin^2~\theta$ $n_p = \sqrt{1.00+sin^2~\theta}$ The index of refraction of the prism is $~~\sqrt{1.00+sin^2~\theta}$
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