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 23 - Ray Optics - Exercises and Problems - Page 693: 77

Answer

See the detailed answer below.

Work Step by Step

From the geometry of the figure below, we can see that angle 1 is equal to angle $\phi$ since the same diagonal line cuts the two parallel lines. And angle 1 is equal to angle 2 since the incident angle is equal to the reflected angle. Thus, the triangle ACF is an isosceles one. And hence, segments FC and fA are equal. $$\overline{FC}=\overline{FA}$$ now if we proved that $\overline{CF}= \overline{CA}/2$, then $f=R/2$. Now we can use the law of cosines, where $$(\overline{FA})^2 =(\overline{CA})^2 +(\overline{CF})^2 -2(\overline{CA})(\overline{CF})\cos\phi $$ Noting that $R=\overline{CA}=\overline{CB}$, $f=\overline{BF}=\overline{CB}-\overline{CF}=R-\overline{FC}$, so $\overline{CF}=R-f$ and that, $\overline{CF}=\overline{FA}$ $$0 =R^2 -2R(R-f)\cos\phi $$ So, $$R^{ \color{red}{\bf\not} 2}=2 \color{red}{\bf\not} R (R-f)\cos\phi $$ $$R=2R\cos\phi -2f\cos\phi$$ Hence, $$f=\dfrac{2R\cos\phi -R}{2\cos\phi}$$ And when $\phi\lt \lt 1$, then $\cos\phi$ approach 1. Thus, $$\boxed{f=\dfrac{R}{2}}$$ Now we know that $\phi$ must be small for some limits to use the law of $f=R/2$
Update this answer!

You can help us out by revising, improving and updating this answer.

Update this answer

After you claim an answer you’ll have 24 hours to send in a draft. An editor will review the submission and either publish your submission or provide feedback.