Fundamentals of Physics Extended (10th Edition)

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

Chapter 36 - Diffraction - Problems - Page 1109: 15a

Answer

$I(\theta)=I_m (\frac{\sin \alpha}{\alpha})^2$ $I_m/2=I_m (\frac{\sin \alpha}{\alpha})^2$ $1/2=(\frac{\sin \alpha}{\alpha})^2$ $1/2=(\frac{\sin^2 \alpha}{\alpha^2})$ $\alpha^2*1/2=\sin^2 \alpha$ We show that $\alpha^2*1/2=\sin^2 \alpha$ when the intensity is one-half that at the center of the pattern

Work Step by Step

We require that the intensity is one-half that at the center of the pattern, ($I=I_m/2$). Now we use this is equation (36-5): $I(\theta)=I_m (\frac{\sin \alpha}{\alpha})^2$ $I_m/2=I_m (\frac{\sin \alpha}{\alpha})^2$ $1/2=(\frac{\sin \alpha}{\alpha})^2$ $1/2=(\frac{\sin^2 \alpha}{\alpha^2})$ $\alpha^2*1/2=\sin^2 \alpha$ So it is true that $\alpha^2*1/2=\sin^2 \alpha$ when the intensity is one-half that at the center of the pattern
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