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 22 - Wave Optics - Exercises and Problems - Page 650: 38

Answer

$500\;\rm nm$

Work Step by Step

We know, in diffraction gratings, that $$d\sin\theta_m=m\lambda$$ Hence, the light’s wavelength is given by $$\lambda=\dfrac{d\sin\theta_m}{m}$$ Plugging the known; $$\lambda=\dfrac{\frac{1\times 10^{-3}}{500}\cdot \sin30^\circ}{m}$$ $$\lambda=\dfrac{1\times10^{-6} }{m}=\dfrac{1000\;\rm nm}{m}$$ We need to find the visible light which is between 400 nm to 700 nm. At $m=1$; $$\lambda =\dfrac{1000\;\rm nm}{1}=1000\;\rm nm$$ which is not in the range of the visible light. At $m=2$; $$\lambda =\dfrac{1000\;\rm nm}{2}=\color{red}{\bf 500}\;\rm nm$$ This is a visible light. At $m=3$; $$\lambda =\dfrac{1000\;\rm nm}{3}= {\bf 333}\;\rm nm$$ which is not in the range of the visible light. moving forward will give us less wavelengths. So that the right answer here is 500 nm only.
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