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A diverging lens with \(f=-30.0 \mathrm{~cm}\) is placed \(15.0 \mathrm{~cm}\) behind a converging lens with \(f=20.0 \mathrm{~cm}\). Where will an object at infinity in front of the converging lens be focused?

Short Answer

Expert verified
Answer: The object will be focused at a distance of \(5.0~cm\) behind the diverging lens.

Step by step solution

01

Find the image position of object due to the converging lens

Since the object is at infinity, the image will be at the focal point of the converging lens. So, the image position due to the converging lens (\(d_{i1}\)) is \(20.0~cm\) behind it.
02

Find the object position for the diverging lens

The object for the diverging lens will be the image formed by the converging lens. We know that the distance between the two lenses is \(15.0~cm\), so the object is \(20.0 - 15.0 = 5.0~cm\) away from the diverging lens. We can denote this distance as \(d_{o2}\).
03

Use Lensmaker's equation for the diverging lens

Lensmaker's equation is given as follows: \(\frac{1}{f} = \frac{1}{d_o} - \frac{1}{d_i}\) For the diverging lens, \(f = -30.0~cm\) and \(d_{o2} = 5.0~cm\). We will now use this equation to find the image position for the diverging lens (\(d_{i2}\)). \(\frac{1}{-30.0} = \frac{1}{5.0} - \frac{1}{d_{i2}}\)
04

Solve for \(d_{i2}\)

We have the equation: \(\frac{1}{-30.0} = \frac{1}{5.0} - \frac{1}{d_{i2}}\) To solve for \(d_{i2}\), we will first subtract \(\frac{1}{5.0}\) from both sides: \(\frac{1}{-30.0} - \frac{1}{5.0} = -\frac{1}{d_{i2}}\) Now we need to find a common denominator for the fractions on the left-hand side of the equation. The common denominator will be \(30.0\): \(\frac{-5-1}{30.0} = -\frac{1}{d_{i2}}\) \(\frac{-6}{30.0} = -\frac{1}{d_{i2}}\) Now we have fractions with the same numerator, so we can easily find \(d_{i2}\): \(d_{i2} = 30.0 \cdot \frac{1}{6} = 5.0~cm\)
05

Final Answer

The final image position is \(5.0~cm\) behind the diverging lens.

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Most popular questions from this chapter

In H.G. Wells's classic story The Invisible Man, a man manages to change the index of refraction of his body to 1.0 ; thus, light would not bend as it enters his body (assuming he is in air and not swimming). If the index of refraction of his eyes were equal to one, would he be able to see? If so, how would things appear?

Two converging lenses with focal lengths \(5.00 \mathrm{~cm}\) and \(10.0 \mathrm{~cm}\), respectively, are placed \(30.0 \mathrm{~cm}\) apart. An object of height \(h=5.00 \mathrm{~cm}\) is placed \(10.0 \mathrm{~cm}\) to the left of the \(5.00-\mathrm{cm}\) lens. What will be the position and height of the final image produced by this lens system?

A telescope has been properly focused on the Sun. You want to observe the Sun visually, but to protect your sight you don't want to look through the eyepiece; rather, you want to project an image of the Sun on a screen \(1.5 \mathrm{~m}\) behind (the original position of) the eyepiece, and observe that. If the focal length of the eyepiece is \(8.0 \mathrm{~cm},\) how must you move the eyepiece?

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A refracting telescope has the objective lens of focal length \(10.0 \mathrm{~m}\). Assume it is used with an eyepiece of focal length \(2.00 \mathrm{~cm}\). What is the magnification of this telescope?

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