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: 34

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$$\color{blue}{\bf [a]}$$ Let's assume that the lenses are simple magnifiers with $M=\dfrac{25\;\rm cm}{f}$. Hence, $$f_{\rm obj}=\dfrac{25}{M_{\rm obj}}\tag 1$$ and, $$f_{\rm eye}=\dfrac{25}{M_{\rm eye}}\tag 2$$ where we know that the magnification of a telescope is given by $$M=-\dfrac{f_{\rm obj}}{f_{\rm eye}}$$ Plugging from (1) and (2), $$M=-\dfrac{\dfrac{25}{M_{\rm obj}}}{\dfrac{25}{M_{\rm eye}}}$$ $$M=-\dfrac{M_{\rm eye}}{M_{\rm obj}}$$ Noting that to maximize the telescope magnification, we should have ${M_{\rm eye}}\gt {M_{\rm obj}}$ So according to the given; $$M=-\dfrac{5}{2}=\color{red}{\bf 2.5}$$ We ignored the negative sign since the magnification is an absolute value (but you still can use it since it means that the magnified image is upside down). $$\color{blue}{\bf [b]}$$ We answered that above in part (a) when we wrote that we should have ${M_{\rm eye}}\gt {M_{\rm obj}}$. Hence, the lens that should be used for the object is the one that has $2.0\times$ magnification. $$\color{blue}{\bf [c]}$$ The minimum length of the telescope is given by the sum of the two focal lengths of the two lenses. $$L=f_{\rm obj}+f_{\rm eye}$$ Plugging from (1) and (2), $$L=\dfrac{25}{M_{\rm obj}}+\dfrac{25}{M_{\rm eye}}$$ Plug the known; $$L=\dfrac{25}{2}+\dfrac{25}{5}=\color{red}{\bf 17.5}\;\rm cm$$
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