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: 42

Answer

a) $1.26\;\rm m$ b) $7\;\rm bright\;fringes$

Work Step by Step

$$\color{blue}{\bf [a]}$$ We know that the distance between the two $m=1$ bright fringes is twice the distance of $y_1$. $$\Delta y=2y_1\tag 1$$ where $y_1$ is the distance of the $m=1$ bright fringe. Recalling that $y_1$ in a diffraction grating is given by $$y_1=L\tan\theta_1\tag 2$$ Now we need to find the angle which is given by $$d\sin\theta_1=(1)\lambda$$ Hence, $$\theta_1=\sin^{-1}\left( \dfrac{\lambda} {d}\right)$$ where $d=1/N$, $$\theta_1=\sin^{-1}\left( {N \lambda} \right)$$ Plugging into (2); $$y_1=L\tan\left[ \sin^{-1}\left( {N \lambda} \right)\right]$$ Plugging into (1); $$\Delta y=2L\tan\left[ \sin^{-1}\left( {N \lambda} \right)\right]$$ Plugging the known; $$\Delta y=2(2)\tan\left[ \sin^{-1}\left( {\frac{600}{10^{-3}} (500\times 10^{-9})} \right)\right]$$ $$\Delta y=\color{red}{\bf 1.26}\;\rm m$$ $$\color{blue}{\bf [b]}$$ We know that the number of bright fringes is determined by the maximum value of $m$, $$\sin\theta_m=\dfrac{m\lambda}{d}= m\lambda N $$ where the right side must be less than 1, so $$ \dfrac{m\lambda}{d}= m(500\times 10^{-9})(600\times 10^3)$$ $$ \dfrac{m\lambda}{d}=\dfrac{3}{10} m $$ At $m=1$, $$ \dfrac{m\lambda}{d}=\dfrac{3}{10} (1)=\bf 0.3\lt 1 $$ At $m=2$, $$ \dfrac{m\lambda}{d}=\dfrac{3}{10} (2)=\bf 0.6\lt 1 $$ At $m=3$, $$ \dfrac{m\lambda}{d}=\dfrac{3}{10} (3)=\bf 0.9\lt 1 $$ At $m=4$, $$ \dfrac{m\lambda}{d}=\dfrac{3}{10} (4)= 1.2\gt 1 $$ So we will get a maximum number of $m=3$. Hence, the total number of bright fringes is 3 on each side (which means 6 bright fringes) plus the central maximum. Therefore, we can get 7 bright fringes only.
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