Physics: Principles with Applications (7th Edition)

Published by Pearson
ISBN 10: 0-32162-592-7
ISBN 13: 978-0-32162-592-2

Chapter 23 - Light: Geometric Optics - General Problems - Page 677: 86

Answer

$1.41\lt n_{prism}\lt1.88$

Work Step by Step

We know that when the reservoir is empty the light experience a total internal reflection toward the sensor. And when there is liquid, some of the light reflects and the other part refracts outside the prism inside the liquid. For total reflection, $$\dfrac{n_2}{n_1}=\sin\theta_c$$ where $n_1$ is for the prism and $n_2$ is for the outside material. Solving for $n_1$; $$n_1=\dfrac{n_2}{\sin\theta_c}\tag1$$ The minimum value of the index of refraction of the prism is given when its hypotenuse is covered by air $$n_{1,minimum}=\dfrac{n_{air}}{\sin\theta_c}$$ From the geometry of the given figure, we can see that the incident angle and the reflected angle are 45$^\circ$. So, $$n_{1,minimum}=\dfrac{1}{\sin45^\circ}=\bf 1.41$$ The maximum value of the index of refraction of the prism is given when its hypotenuse is covered by the liquid (water). $$n_{1,maximum }=\dfrac{n_{water}}{\sin\theta_c}$$ From the geometry of the given figure, we can see that the incident angle and the reflected angle are 45$^\circ$. So, $$n_{1,maximum }=\dfrac{1.33}{\sin45^\circ}=\bf 1.88$$ Therefore, and from all the above, $$\boxed{1.41\lt n_{prism}\lt1.88}$$
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