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 1009: 97

Answer

$\theta = cos^{-1}~\sqrt{\frac{p}{50}}$

Work Step by Step

Let $I_0$ be the original intensity of the light. Since the light is initially unpolarized, half the intensity will be transmitted through the first polarizing sheet. $I_1 = \frac{1}{2}I_0$ We can find an expression for $I_2$: $I_2 = I_1~cos^2~\theta^{\circ}$ $I_2 = \frac{1}{2}I_0~cos^2~\theta$ We can find $\theta$: $I_2 = \frac{1}{2}I_0~cos^2~\theta = \frac{p}{100}~I_0$ $cos^2~\theta = \frac{p}{50}$ $cos~\theta = \sqrt{\frac{p}{50}}$ $\theta = cos^{-1}~\sqrt{\frac{p}{50}}$
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