Physics for Scientists and Engineers: A Strategic Approach with Modern Physics (3rd Edition)

Published by Pearson
ISBN 10: 0321740904
ISBN 13: 978-0-32174-090-8

Chapter 23 - Ray Optics - Exercises and Problems - Page 692: 56

Answer

$3$ cm below the surface.

Work Step by Step

In this situation, the object, which is the air bubble, is behind the refracted surface of the sphere and it faces a concave surface. Thus, $R=-3$ cm. And since the air bubble is just in the middle, $s=3$ cm. Recalling for spherical surfaces that object and image distances are related by $$\dfrac{n_1}{s}+\dfrac{n_2}{s'}=\dfrac{n_2-n_1}{R}$$ where $n_1$ here is for zircon and it is 2.18 [see table 23.1], while $n_2$ is for air and is it 1.0. Now we need to plug the known and solve for $s'$, $$\dfrac{2.18}{3}+\dfrac{1}{s'}=\dfrac{1-2.18}{-3}$$ Hence, $$s'=\color{red}{\bf-3}\;{\rm cm}=R$$ This means that when the bubble is at the center, it appears to be exactly at the center.
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