Physics: Principles with Applications (7th Edition)

Published by Pearson
ISBN 10: 0-32162-592-7
ISBN 13: 978-0-32162-592-2

Chapter 23 - Light: Geometric Optics - General Problems - Page 677: 87

Answer

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Work Step by Step

a) For the first lens, we know that $$\dfrac{1}{f_1}=\dfrac{1}{d_{o1}}+\dfrac{1}{d_{i1}}$$ $i$ for image and $o$ for object. When two lenses are placed in contact, the negative image of the first lens represents the object of the second lens. $$ \dfrac{1}{d_{i1}}=\dfrac{1}{f_1}-\dfrac{1}{d_{o1}}$$ Thus, $$ \dfrac{1}{d_{i1}}=\dfrac{1}{f_1}-\dfrac{1}{d_{o1}}=\dfrac{-1}{d_{o2}} $$ And hence, $$ \dfrac{ 1}{d_{o2}} =-\left[\dfrac{1}{f_1}-\dfrac{1}{d_{o1}}\right]\tag 1$$ For the second lens, we know that $$\dfrac{1}{f_2}=\dfrac{1}{d_{o2}}+\dfrac{1}{d_{i2}}$$ Plugging from (1); $$\dfrac{1}{f_2}=-\left[\dfrac{1}{f_1}-\dfrac{1}{d_{o1}}\right]+\dfrac{1}{d_{i2}}$$ $$\dfrac{1}{f_2}+\dfrac{1}{f_1}=\overbrace{\dfrac{1}{d_{o1}} +\dfrac{1}{d_{i2}}}^{\dfrac{1}{f_T}}$$ Therefore, $$\boxed{\dfrac{1}{f_T}=\dfrac{1}{f_1}+\dfrac{1}{f_2}}$$ --- b) We know that the power of the lens is given by $$P=\dfrac{1}{f}$$ Thus, from the boxed formula above, $$\boxed{P_T=P_1+P_2}$$
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