/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 78 A 1.5-cm-tall object is 90 \(\ma... [FREE SOLUTION] | 91影视

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A 1.5-cm-tall object is 90 \(\mathrm{cm}\) in front of a diverging lens that has a \(45 \mathrm{cm}\) focal length. Use ray tracing to find the position and height of the image. To do this accurately, use a ruler or paper with a grid. Determine the image distance and image height by making measurements on your diagram.

Short Answer

Expert verified
The image formed by the diverging lens is located 90cm in front of it, on the same side as the object, and is of the same size (1.5cm) as the object, but upright. This is a virtual image.

Step by step solution

01

Apply the lens formula

The lens formula is \[1/f = 1/v - 1/u\]. We can rearrange this to find \(v\): \[1/v = 1/f + 1/u\]. Substituting \(f = -45cm\) and \(u = -90cm\), \[1/v = -1/45 - 1/(-90) = -1/90\]. Therefore \(v = -90cm\]. This means the image is 90cm in front of the lens, on the same side as the object.
02

Apply the magnification formula

The magnification formula is \(m = -v/u = h'/h\), where \(h'\) is the image height. Rearranging, we have \(h' = mh\). Our magnification is \(m = v/u = -90/-90 = 1\). Substituting this into the equation, the height of the image is \(h' = 1 * 1.5cm = 1.5cm\). The positive height means the image is upright.
03

Interpret the results

The image is located 90cm in front of the lens, on the same side as the object. This would appear to an observer as if the light were coming from this position behind the lens. We also found that the image height is the same as the object height, which means the image is the same size as the object, but upright. For a diverging lens, this is a virtual image - it cannot be projected on a screen.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Lens Formula
Understanding the lens formula is critical for predicting how lenses will affect light passing through them. The formula \[\frac{1}{f} = \frac{1}{v} - \frac{1}{u}\]is the foundation for finding where an image will form relative to a lens. Here, \(f\) represents the focal length of the lens, \(v\) is the image distance from the lens, and \(u\) is the object distance from the lens.

To apply the lens formula for a diverging lens, we note that its focal length \(f\) is negative because diverging lenses spread out light rays. Similarly, the object distance \(u\) is negative if the object is placed in front of the lens, following sign convention in optics. To find the image distance \(v\), you simply rearrange the formula:
\[\frac{1}{v} = \frac{1}{f} + \frac{1}{u}\]
Once you substitute the given values and solve for \(v\), you can determine the location of the image which, for a diverging lens, will always be virtual and on the same side as the object.
Ray Tracing
Ray tracing is a method used to visually determine the path of light through lenses and mirrors. It involves drawing a set of principal rays that follow specific predictable paths when they strike a lens. In the case of a diverging lens, the principal rays include:
  • A ray parallel to the principal axis, which will diverge as if it came from the focal point on the same side of the lens after passing through the lens.
  • A ray passing through the center of the lens, which will continue straight without bending.
  • A ray aiming towards the focal point on the far side of the lens, which will emerge parallel to the principal axis.

By extending these rays backward, they will appear to come from a single point, locating the virtual image. The intersection of the rays gives you both the position and height of the image. Using a ruler or grid paper helps in making accurate ray tracing diagrams, which is essential for visualizing the process of image formation.
Image Magnification
Image magnification is a measure of how a lens enlarges or reduces the size of an image compared to the object. It's defined by the formula:
\[ m = \frac{-v}{u} = \frac{h'}{h} \]
where \(m\) is the magnification, \(v\) is the image distance, \(u\) is the object distance, \(h'\) is the image height, and \(h\) is the object height. Negative magnification indicates an inverted image, while positive magnification suggests an upright image. For the exercise at hand, the magnification turned out to be 1, meaning the image is the same size as the object. By understanding how to use and interpret the magnification formula, you can not only determine the size of the image but also infer its orientation (upright or inverted).
Virtual Image
A virtual image is an image formed by a lens or mirror that appears to be in a location from which light does not actually come. For diverging lenses, the rays diverge after passing through the lens and only appear to originate from a common point when traced back. Unlike a real image, a virtual image cannot be projected onto a screen because the light rays don't actually converge.

In the context of our exercise, the diverging lens produces a virtual image that is the same size as the object and located 90cm in front of the lens, which is also upright. Virtual images produced by diverging lenses are always found on the same side as the object and are always upright. Knowing this characteristic helps in predicting the nature of the image without complex calculations, making it a valuable concept in optics.

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Most popular questions from this chapter

In order to start a fire, a camper turns a lens toward the sun to focus its rays on a piece of wood. The lens has a \(10 \mathrm{cm}\) focal length. Draw a ray diagram of the lens and the incoming light rays to show where the wood should be placed for the best effect.

A biologist keeps a specimen of his favorite beetle embedded in a cube of polystyrene plastic. The hapless bug appears to be \(2.0 \mathrm{cm}\) within the plastic. What is the beetle's actual distance beneath the surface?

You are standing \(1.5 \mathrm{m}\) from a mirror, and you want to use a classic camera to take a photo of yourself. This camera requires you to select the distance of whatever you focus on. What distance do you choose?

A point source of light illuminates an aperture \(2.00 \mathrm{m}\) away. A 12.0 -cm-wide bright patch of light appears on a screen \(1.00 \mathrm{m}\) behind the aperture. How wide is the aperture?

There is an interesting optical effect you have likely noticed while driving along a flat stretch of road on a sunny day. A small, distant dip in the road appears to be filled with water. You may even see the reflection of an oncoming car. But, as you get closer, you find no puddle of water after all; the shimmering surface vanishes, and you see nothing but empty road. It was only a mirage, the name for this phenomenon. The mirage is due to the different index of refraction of hot and cool air. The actual bending of the light rays that produces the mirage is subtle, but we can make a simple model as follows. When air is heated, its density decreases and so does its index of refraction. Consequently, a pocket of hot air in a dip in a road has a lower index of refraction than the cooler air above it. Incident light rays with large angles of incidence (that is, nearly parallel to the road, as shown in Figure P18.83) experience total internal reflection. The mirage that you see is due to this reflection. As you get nearer, the angle goes below the critical angle and there is no more total internal reflection; the 鈥渨ater鈥 disappears! Which of these changes would allow you to get closer to the mirage before it vanishes? A. Making the pocket of hot air nearer in temperature to the air above it B. Looking for the mirage on a windy day, which mixes the air layers C. Increasing the difference in temperature between the pocket of hot air and the air above it D. Looking at it from a greater height above the ground

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