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The focal length of a simple magnifier is \(8.00 \mathrm{~cm}\). Assume the magnifier to be a thin lens placed very close to the eye. (a) How far in front of the magnifier should an object be placed if the image is formed at the observer's near point, \(25.0 \mathrm{~cm}\) in front of her eye? (b) If the object is \(1.00 \mathrm{~mm}\) high, what is the height of its image formed by the magnifier?

Short Answer

Expert verified
(a) The object should be 6.06 cm from the magnifier. (b) The image is 4.13 mm high.

Step by step solution

01

Understanding the Lens Formula

We know the lens formula is given by: \( \frac{1}{f} = \frac{1}{d_o} + \frac{1}{d_i} \), where \( f \) is the focal length of the lens, \( d_o \) is the object distance, and \( d_i \) is the image distance. Here, \( f = 8.00 \) cm and \( d_i = -25.0 \) cm (negative because the image forms on the same side as the object for a virtual image). Our objective is to find \( d_o \).
02

Solving for Object Distance

Rearrange the lens formula to solve for \( d_o \): \( \frac{1}{d_o} = \frac{1}{f} - \frac{1}{d_i} \). Substituting the given values: \( \frac{1}{d_o} = \frac{1}{8.00} - \frac{1}{-25.0} \). Calculating the right hand side gives: \( \frac{1}{d_o} = \frac{1}{8.00} + \frac{1}{25.0} = \frac{25.0 + 8.00}{200.0} = \frac{33.0}{200.0} \). Thus, \( d_o = \frac{200.0}{33.0} \approx 6.06 \text{ cm} \).
03

Understanding Magnification

The magnification \( m \) is given by the formula \( m = -\frac{d_i}{d_o} \). The negative sign signifies that the image is virtual and upright as compared to the object. We must also relate this to the height of the image \( h_i \). The relation is \( m = \frac{h_i}{h_o} \), where \( h_o = 1.00 \) mm is the object height.
04

Calculating Image Height

Substitute the given values into the magnification formula to find the image height \( h_i \). Using \( m = -\frac{d_i}{d_o} \), we get \( m = -\frac{-25.0}{6.06} \approx 4.13 \). Thus, \( h_i = m \times h_o = 4.13 \times 1.00 \) mm. Therefore, \( h_i \approx 4.13 \) mm.

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Key Concepts

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

Focal Length
In optics, focal length is a key concept when understanding how lenses focus light to form images. The focal length (\( f \)) of a lens is defined as the distance from the lens to the point where parallel rays of light converge or appear to diverge after passing through the lens. Depending on the type of lens, this point can be real or virtual. For converging lenses, it is a positive value, indicating the real focal point is on the opposite side of the incoming light. Conversely, for diverging lenses, the focal length is negative, suggesting the focal point is virtual and on the same side as the incoming light.

Knowing the focal length is crucial for applications like a simple magnifier, where the lens needs a specific focal length, such as 8 cm in the exercise, to effectively magnify objects placed at a certain distance from the lens. This parameter determines how the lens will bend light, affecting image size and clarity.
Lens Formula
The lens formula is a fundamental equation in optics used to relate the object distance (\( d_o \)), image distance (\( d_i \)), and focal length (\( f \)). It is given by:
\[ \frac{1}{f} = \frac{1}{d_o} + \frac{1}{d_i} \]

This formula provides a mathematical way to calculate how far an object should be from the lens to form an image at a desired location. In practice, it helps in designing optical systems like cameras and projectors.
  • When solving problems, ensure the sign conventions are followed: real distances are positive, while virtual distances are negative.
  • In the exercise, since we are dealing with a virtual image formed at the observer's near point, the image distance is negative.
By substituting the known values into the formula, one can find the object distance (\( d_o \)) needed for the image to form at the specified position.
Image Magnification
Image magnification describes how much larger or smaller an image is compared to the object itself. This concept is especially important for devices like magnifiers, which are used to produce a larger view of small objects. Magnification (\( m \)) is determined using the formula:
\[ m = -\frac{d_i}{d_o} \]

The negative sign indicates that the image is virtual and upright. In magnification problems, it is also common to calculate the image height (\( h_i \)), using:
  • \( m = \frac{h_i}{h_o} \)
  • where \( h_o \) is the object height.
In this exercise, with an object height of 1 mm, you can determine that the image is approximately 4.13 mm high, thanks to a magnification factor of approximately 4.13. This means the image is over four times larger than the original object.
Virtual Image
A virtual image in optics is an image formed by diverging light rays that appear to come from a certain point. Unlike a real image, which can be projected onto a screen, a virtual image cannot be captured in this way. Instead, it is visible when looking through an optical device.
A good example is using a magnifying lens to see an enlarged version of a small object. The image you see through the magnifier appears to be on the same side as the object itself. This is typical of a virtual image. In the exercise, the virtual image is formed at the observer's near point, at 25 cm from the eye. This allows detailed examination of small objects by effectively enlarging them to make them easier to see.
  • Virtual images are created by diverging lenses or by positioning objects within the focal length of converging lenses.
  • These images are always upright and cannot be projected onto a surface.
Understanding virtual images is fundamental for using optical devices appropriately.

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Most popular questions from this chapter

A frog can see an insect clearly at a distance of \(10 \mathrm{~cm}\). At that point the effective distance from the lens to the retina is \(8 \mathrm{~mm} .\) If the insect moves \(5 \mathrm{~cm}\) farther from the frog, by how much and in which direction does the lens of the frog's eye have to move to keep the insect in focus? A. \(0.02 \mathrm{~cm},\) toward the retina B. \(0.02 \mathrm{~cm}\), away from the retina C. \(0.06 \mathrm{~cm}\), toward the retina D. \(0.06 \mathrm{~cm}\), away from the retina

A \(135 \mathrm{~mm}\) telephoto lens for a \(35 \mathrm{~mm}\) camera has \(f\) -stops that range from \(f / 2.8\) to \(f / 22 .\) (a) What are the smallest and largest aperture diameters for this lens? What is the diameter at \(f / 11 ?\) (b) If a \(50 \mathrm{~mm}\) lens had the same \(f\) -stops as the telephoto lens, what would be the smallest and largest aperture diameters for that lens? (c) At a given shutter speed, what is the ratio of the greatest to the smallest light intensity of the film image? (d) If the shutter speed for correct exposure at \(f / 22\) is \(1 / 30 \mathrm{~s},\) what shutter speed is needed at \(f / 2.8 ?\) Calculate \(m_{1}\) and \(M_{2}\) for the two lenses and do not make the approximation that leads to Equation 25.4

A certain digital camera having a lens with focal length \(7.50 \mathrm{~cm}\) focuses on an object \(1.85 \mathrm{~m}\) tall that is \(4.25 \mathrm{~m}\) from the lens. (a) How far must the lens be from the sensor array? (b) How tall is the image on the sensor array? Is it upright or inverted? Real or virtual? (c) An SLR digital camera often has pixels measuring \(8.0 \mu \mathrm{m} \times 8.0 \mu \mathrm{m}\). How many such pixels does the height of this image cover?

In one form of cataract surgery, the person's natural lens, which has become cloudy, is replaced by an artificial lens. The refracting properties of the replacement lens can be chosen so that the person's eye focuses on distant objects. But there is no accommodation, and glasses or contact lenses are needed for close vision. What is the power, in diopters, of the corrective contact lenses that will enable a person who has had such surgery to focus on the page of a book at a distance of \(24 \mathrm{~cm} ?\)

The crystalline lens of the human eye is double convex and has a typical range of optical power from 115 diopters to 150 diopters. (a) What is the range of focal lengths the eye can achieve? (b) At minimum power, where does it focus the image of a very distant object? (c) At maximum power, where does it focus the image of an object at the near point of \(25 \mathrm{~cm} ?\)

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