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A converging lens forms an image of an \(8.00-\) mm-tall real object. The image is 12.0 \(\mathrm{cm}\) to the left of the lens, 3.40 \(\mathrm{cm}\) tall, and erect. (a) What is the focal length of the lens? (b) Where is the object located? (c) Draw a principal-ray dia- gram for this situation.

Short Answer

Expert verified
(a) The focal length of the lens is -2.28 cm. (b) The object is 2.82 cm to the left of the lens.

Step by step solution

01

Analyze Given Information for Part (a)

The image is on the same side as the object, which is atypical for a real image formed by a converging lens. Given the image distance \(d_i = -12.0\, \text{cm}\), since it's to the left, and the height of the image is 3.40 cm, we can note that the image is erect and magnified.
02

Use the Magnification Formula for Part (a)

Magnification \(m\) is given by \(m = \frac{h_i}{h_o} = \frac{d_i}{d_o}\). Here, \(h_i = 3.40\, \text{cm}\) and \(h_o = 0.80\, \text{cm}\). Therefore, \(m = \frac{3.40}{0.80} = 4.25\). Using \(m = \frac{-d_i}{d_o}\), substitute \(d_i = -12.0\, \text{cm}\) to find \(d_o\): \(d_o = \frac{-12.0}{4.25}\, \text{cm} = -2.82\, \text{cm}\).
03

Apply Lens Formula to Find Focal Length for Part (a)

Use the lens formula, \(\frac{1}{f} = \frac{1}{d_o} + \frac{1}{d_i}\). Substitute \(d_o = -2.82\, \text{cm}\) and \(d_i = -12.0\, \text{cm}\): \(\frac{1}{f} = \frac{1}{-2.82} + \frac{1}{-12.0}\). Calculate \(\frac{1}{f} = -0.355 + (-0.083) = -0.438\). Thus, \(f = -2.28\, \text{cm}\).
04

Confirm the Object Location for Part (b)

From Step 2, the calculated object distance is \(d_o = -2.82\, \text{cm}\). Thus, the object is located 2.82 cm to the left of the lens, which confirms the previous result.

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Key Concepts

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

Converging Lens
A converging lens, also known as a convex lens, is a piece of transparent material, like glass or plastic, that is thicker at the middle than at the edges. These lenses are commonly used to focus light to a point. When parallel rays of light pass through a converging lens, they bend towards the lens's focal point. This ability makes converging lenses essential in various optical devices, such as cameras, magnifying glasses, and eyeglasses for correcting farsightedness.

A key characteristic of a converging lens is its focal length - the distance from the lens to the focal point where light rays meet. The focus of the converging lens is where the image is formed, which can be either real or virtual depending on the position of the object relative to the lens. In our exercise, the calculations revealed a real image being formed to the left of the lens, meaning the focal point lies beyond the object on the same side of the light's entry.
Magnification Formula
Magnification in optics is a measure of how much larger or smaller an image is compared to the object itself. It is a crucial concept when dealing with lenses because it helps determine the image size and orientation.

The magnification formula is \( m = \frac{h_i}{h_o} \ = \frac{d_i}{d_o} \), where:
  • \( h_i \) is the height of the image.
  • \( h_o \) is the height of the object.
  • \( d_i \) is the distance from the image to the lens.
  • \( d_o \) is the distance from the object to the lens.
Using this formula, we can determine how the lens affects the object's image size. In the exercise, the magnification was calculated as 4.25, indicating that the image is 4.25 times larger than the object and erect, as explained by the positive value.
Lens Formula
The lens formula relates the object distance \( d_o \), image distance \( d_i \), and the focal length \( f \) of a lens. It is expressed as:\[ \frac{1}{f} = \frac{1}{d_o} + \frac{1}{d_i}\]This formula is fundamental when analyzing the behavior of lenses, as it helps in finding either the object distance, image distance, or focal length when the other two quantities are known.

Applying the formula involves simple algebraic manipulation and substitution of known values. For the given exercise, the lens formula was used to calculate the focal length as \( f = -2.28\, \text{cm} \), implying a negative value for a virtual image scenario typical in some cases with converging lenses.
Principal-Ray Diagram
A principal-ray diagram is an excellent tool for visually understanding how lenses form images. It graphically represents the paths of a few special rays - generally three - that are easy to trace. These rays include:
  • The ray parallel to the principal axis, refracted through the focal point on the opposite side.
  • The ray passing through the center of the lens, which continues straight without bending.
  • The ray passing through the focal point on the object side, refracted parallel to the principal axis on the opposite side.
Drawing such diagrams requires knowing the focal points and distances from the object and image to the lens. For our exercise, creating a diagram helps to confirm that both object and image locations align with the solutions provided—showcasing how light rays converge to form an upright and magnified image, thus supporting our earlier calculations.

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Most popular questions from this chapter

A concave mirror is to form an image of the filament of a headlight lamp on a screen 8.00 m from the mirror. The filament is 6.00 mm tall, and the image is to be 36.0 \(\mathrm{cm}\) tall. (a) How far in front of the vertex of the mirror should the filament be placed? (b) To what radius of curvature should you grind the mirror?

\(\bullet \mathrm{A}\) zoo aquarium has transparent walls, so that spectators on both sides of it can watch the fish. The aquarium is 5.50 \(\mathrm{m}\) across, and the spectators on both sides of it are standing 1.20 \(\mathrm{m}\) from the wall. How far away do spectators on one side of the aquarium appear to those on the other side? (Ignore any refraction in the walls of the aquarium.)

\(\cdot\) To a person swimming 0.80 \(\mathrm{m}\) beneath the surface of the water in a swimming pool, the diving board directly overhead appears to be a height of 5.20 \(\mathrm{m}\) above the swimmer. What is the actual height of the diving board above the surface of the water?

\(\cdot\) The left end of a long glass rod 8.00 \(\mathrm{cm}\) in diameter and with an index of refraction of 1.60 is ground and polished to a convex hemispherical surface with a radius of 4.00 \(\mathrm{cm} .\) An object in the form of an arrow 1.50 \(\mathrm{mm}\) tall, at right angles to the axis of the rod, is located on the axis 24.0 \(\mathrm{cm}\) to the left of the vertex of the convex surface. Find the position and height of the image of the arrow formed by paraxial rays inci- dent on the convex surface. Is the image erect or inverted?

An object is placed 18.0 \(\mathrm{cm}\) from a screen. (a) At what two points between object and screen may a converging lens with a 3.00 \(\mathrm{cm}\) focal length be placed to obtain an image on the screen? (b) What is the magnification of the image for each position of the lens?

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