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(II) \(\mathrm{A}-8.00\) -D lens is held 12.5 \(\mathrm{cm}\) from an ant 1.00 \(\mathrm{mm}\) high. Describe the position, type, and height of the image.

Short Answer

Expert verified
The image is virtual, at infinity, with unquantifiable height.

Step by step solution

01

Identify the focal length of the lens

The lens power is given by the formula \( ext{Power} = \frac{1}{ ext{focal length in meters}} \). Given \( ext{Power} = -8.00 \) D, we need to find the focal length (\( f \)) in meters. Use \( f = \frac{1}{ ext{Power}} = \frac{1}{-8.00} \approx -0.125 \) meters, or \(-12.5\) cm.
02

Apply the lens formula

The lens formula is \( \frac{1}{f} = \frac{1}{v} - \frac{1}{u} \), where \( v \) is the image distance and \( u \) is the object distance. The object distance \( u = -12.5 \) cm because it is on the same side as the light source for lenses. Using \( f = -12.5 \) cm: \[ \frac{1}{-12.5} = \frac{1}{v} - \frac{1}{-12.5} \]. Solve for \( v \).
03

Calculate the image distance (v)

Rearrange to find \( v \): \[ \frac{1}{v} = \frac{1}{-12.5} - \frac{1}{-12.5} = 0 \]. This implies that \( v \to \infty \). Therefore, the image formed is at infinity.
04

Determine the type of image

Since the image distance \( v \to \infty \), the image formed by the lens is virtual. This is because the image cannot be formed on a screen when using a diverging lens with this configuration.
05

Calculate the magnification and height of the image

Magnification is given by \( m = \frac{v}{u} \), which leads to an indeterminate form here since \( v \to \infty \). Practically, the image of the object would be very small or nonexistent visually. The height of the image technically cannot be computed accurately here.

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Key Concepts

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

Image Distance
In optics, the image distance is the distance between the image formed by a lens and the lens itself. It is denoted by the symbol \( v \). Determining the image distance involves using the lens formula, which relates the object distance, the focal length of the lens, and the image distance. The lens formula is given by:
  • \( \frac{1}{f} = \frac{1}{v} - \frac{1}{u} \)
Here, \( f \) is the focal length, \( v \) is the image distance, and \( u \) is the object distance.
In our specific example, both the focal length and the object distance are \(-12.5\) cm. This leads to a calculation where the reciprocal values cancel each other out.
As a result, the fraction becomes zero, meaning that the image distance \( v \) becomes infinite \( v \to \infty \). This indicates that the image is formed at infinity, which is an important aspect of understanding lens behavior.
Virtual Image
A virtual image is an image that cannot be projected on a screen. It is formed when the rays of light appear to diverge from a point. Unlike real images, virtual images form on the same side of the lens as the object.
In a typical setup involving a diverging lens, the image distance may appear as negative in calculations, reinforcing the idea of a virtual image.
In the described exercise, the image is said to be at infinity. Even though it may not seem intuitive, this scenario indeed generates a virtual image. Such images cannot be captured on a screen because the light does not actually converge to form a real point.
  • Virtual images are always upright, not inverted.
  • They generally appear smaller than the actual object.
These concepts explain why, in practical terms, the virtual image described would not visibly manifest in a way that makes the object appear large or prominent.
Magnification
Magnification is a measure of how much larger or smaller an image is compared to the object itself. It is calculated using the formula:
  • \( m = \frac{v}{u} \)
Here, \( m \) represents magnification, \( v \) is the image distance, and \( u \) is the object distance.
In practical scenarios, magnification informs us if an object will appear larger or smaller when viewed through a lens.
For our exercise, the problem becomes interesting because \( v \to \infty \). This suggests the magnification is indeterminate. However, without an actual focus and given the virtual nature of the image, this typically means that the magnification effect is negligible.
  • A positive magnification value indicates the image is upright.
  • A negative value typically means the image is inverted, but this is absent in virtual images.
Due to the complex interplay of image distance and the type of lens, the image can't be visually appreciated as larger or smaller.

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Most popular questions from this chapter

(II) A person struggles to read by holding a book at arm's length, a distance of \(55 \mathrm{~cm}\) away. What power of reading glasses should be prescribed for her, assuming they will be placed \(2.0 \mathrm{~cm}\) from the eye and she wants to read at the "normal" near point of \(25 \mathrm{~cm} ?\)

A \(200-\mathrm{mm}\) -focal-length lens can be adjusted so that it is \(200.0 \mathrm{~mm}\) to \(206.4 \mathrm{~mm}\) from the film. For what range of object distances can it be adjusted?

(I) A microscope uses an eyepiece with a focal length of \(1.50 \mathrm{~cm}\). Using a normal eye with a final image at infinity, the barrel length is \(17.5 \mathrm{~cm}\) and the focal length of the objective lens is \(0.65 \mathrm{~cm}\). What is the magnification of the microscope?

(II) An achromatic lens is made of two very thin lenses, placed in contact, that have focal lengths \(f_{1}=-28 \mathrm{~cm}\) and \(f_{2}=+25 \mathrm{~cm} .\) (a) Is the combination converging or diverging? (b) What is the net focal length?

(II) A converging lens of focal length \(f=12 \mathrm{~cm}\) is being used by a writer as a magnifying glass to read some fine print on his book contract. Initially, the writer holds the lens above the fine print so that its image is at infinity. To get a better look, he then moves the lens so that the image is at his \(25-\mathrm{cm}\) near point. How far, and in what direction (toward or away from the fine print) did the writer move the lens? Assume the writer's eye is adjusted to remain always very near the magnifying glass.

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