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 - Search and Learn - Page 678: 5

Answer

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Work Step by Step

The author needs us to justify that the image distance is positive for a real image and negative for a virtual image. He asks us to use any figures we need, so we will use figures (23–39), (23–40), and (23–43) in our textbook. We have here 3 cases: 1) When we have a diverging lens. 2) When we have a converging lens: a) when $d_o\gt f$ b) when $d_o\lt f$ In these 3 cases, we will use the same formula of $$\dfrac{1}{f}=\dfrac{1}{d_o}+\dfrac{1}{d_i}$$ And since we need to find the image distance for the three cases, we need to solve for $d_i$. $$\dfrac{1}{f}-\dfrac{1}{d_o}=\dfrac{1}{d_i}$$ $$d_i=\left[\dfrac{1}{f}-\dfrac{1}{d_o}\right]^{-1}\tag 1$$ 1) In the first case, as we see in figure (23–39); We can see that $d_o\gt f$ and we know from the first law of sign conventions that the focal length is negative for diverging lenses, so $f\lt 0$. Plugging these data into (1) by plugging some numbers to see if the final result is negative or positive. Let's assume that the focal length is 5 cm and that the object is 6 cm. Thus; $$d_i=\left[\dfrac{1}{-5}-\dfrac{1}{6}\right]^{-1}=\bf -2.73\;\rm cm$$ And since the image here is virtual, so it is obvious that for the virtual images the image distances must be negative. 2-a) In the second case, as we see in figure (23–40); We can see that $d_o\gt f$ and we know from the first law of sign conventions that the focal length is positive for converging lenses, so $f\gt 0$. Plugging these data into (1) by plugging some numbers to see if the final result is negative or positive. Let's assume that the focal length is 5 cm and that the object is 6 cm. Thus; $$d_i=\left[\dfrac{1}{5}-\dfrac{1}{6}\right]^{-1}=\bf +30\;\rm cm$$ And since the image here is real, so it is obvious that for the real images the image distances must be positive. 2-b) In the third case, as we see in figure (23–43); We can see that $d_o\lt f$ and we know from the first law of sign conventions that the focal length is positive for converging lenses, so $f\gt 0$. Plugging these data into (1) by plugging some numbers to see if the final result is negative or positive. Let's assume that the focal length is 5 cm and that the object is 4 cm. Thus; $$d_i=\left[\dfrac{1}{5}-\dfrac{1}{4}\right]^{-1}=\bf -20\;\rm cm$$ And since the image here is virtual, so it is obvious that for the virtual images the image distances must be negative.
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