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 24 - Optical Instruments - Exercises and Problems - Page 714: 37

Answer

$0.462\;\rm cm$

Work Step by Step

First of all, we need to find the focal lengths of the two lenses, where the magnification of the objective lens is given by $$m_{\rm obj}=\dfrac{-L}{f_{\rm obj}}$$ So, $$f_{\rm obj}=\dfrac{-L}{m_{\rm obj}}=\dfrac{18.0}{40}=\bf 0.45\;\rm cm$$ we neglected the negative sign since we are dealing now with lengths. The magnification of the eye lens is given by $$M_{\rm eye}=\dfrac{25\;\rm cm}{f_{\rm eye}} $$ So, $$f_{\rm eye}=\dfrac{25\;\rm cm}{f_{\rm eye}}=\dfrac{25}{20}=\bf 1.25\;\rm cm$$ Now we have the focal length of the objective lens, and we can get the image position. For a relaxed eye, the image of the objective lens must be at the focal point of the eye lens. Thus, $$s'=L-f_{\rm eye}=18-1.25=\bf 16.75\;\rm cm$$ Now we can easily find the position of the sample (the object) by using the thin lens formula. $$\dfrac{1}{f_{\rm obj}}=\dfrac{1}{s}+\dfrac{1}{s'}$$ Hence, $$s=\left[ \dfrac{1}{f_{\rm obj}}-\dfrac{1}{s'} \right]^{-1}$$ $$s=\left[ \dfrac{1}{0.45}-\dfrac{1}{16.75} \right]^{-1}$$ $$s=\color{red}{\bf 0.462}\;\rm cm$$ We can see that $s\approx f_{\rm obj}$
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