/*! 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 33 =A converging lens forms an imag... [FREE SOLUTION] | 91Ó°ÊÓ

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=A converging lens forms an image of an \(8.00-\mathrm{mm}\) -tall real object. The image is \(12.0 \mathrm{~cm}\) to the left of the lens, \(3.40 \mathrm{~cm}\) tall, and erect. What is the focal length of the lens? Where is the object located?

Short Answer

Expert verified
The focal length of the lens is \(3.36\,cm\), and the object is located \(5.1\,cm\) to the left of the lens.

Step by step solution

01

Determine the magnification

First we need to use the magnification of the lens formula to determine the object distance (d_o). The magnification of a lens (\(m\)) is given by the ratio of image height (\(h_i\)) to the object height (\(h_o\)) and is also equal to the negative ratio of the image distance (\(d_i\)) to the object distance (\(d_o\)). Therefore, the object distance can be calculated as follows: \(d_o = -m \cdot d_i\). Here, \(m = h_i/h_o = 3.40\,mm / 8\,mm = 0.425\) and \(d_i = -12\,cm\) (negative because the image is to the left of the lens). Thus, \(d_o = -0.425 \cdot -12\,cm = 5.1\,cm\).
02

Apply the lens maker's formula

Next, we use the object distance (d_o) in the lens maker's formula to calculate the focal length (f). The lens maker's formula is \(1/f = 1/d_o - 1/d_i\). By substituting the values we found earlier (\(d_o = 5.1\,cm\) and \(d_i = -12\,cm\)), we get \(1/f = 1/5.1 - 1/-12 = 0.298 \,cm^{-1}\). Thus, the focal length of the lens, \(f\), is the reciprocal of this value, \(f = 1/0.298 = 3.36\,cm\).
03

Interpret the result

The positive focal length, \(f = 3.36\,cm\), indicates a converging lens, consistent with including that in the problem. The location of the object, \(d_o = 5.1\,cm\) to the left of the lens, is realistic for a converging lens. The magnification \(m = 0.425\) which is less than 1, corresponds to the reduction in size of the image \(3.40\,mm\) compared to the object \(8.00\,mm\).

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Key Concepts

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

Lens Magnification Formula
Understanding the lens magnification formula is crucial for solving optical problems involving lenses. Magnification, denoted as \(m\), is the measure of how much larger or smaller the image appears compared to the object itself. For a lens, this formula can be expressed as \(m = \frac{h_i}{h_o}\) where \(h_i\) is the height of the image and \(h_o\) is the height of the object.

In the context of our problem, the image height is given as \(3.40 \text{mm}\) and the object height as \(8.00 \text{mm}\). By applying the formula, \(m = \frac{3.40 \text{mm}}{8.00 \text{mm}} = 0.425\), we find that the image is smaller than the object, indicating that the image is reduced in size. Another way to express magnification is by the ratio of the image distance (\(d_i\)) to the object distance (\(d_o\)), with the image distance taken as negative if the image is formed on the same side of the lens as the object. This additional understanding helps in comprehensively solving lens-related problems and shows that magnification is a fundamental concept in optics as it connects the physical sizes of objects and their images with the distances they are from the lens.
Lens Maker's Formula
The lens maker’s formula is pivotal for determining the focal length of a lens, which is an essential characteristic that affects how the lens focuses light. The formula is given by \(1/f = (1/d_o) - (1/d_i)\), where \(f\) is the focal length, \(d_o\) is the object distance, and \(d_i\) is the image distance. A positive focal length typically indicates a converging lens, while a negative focal length would indicate a diverging lens.

In our specific problem, we're tasked with finding the focal length for a converging lens. By substituting known values of \(d_o = 5.1 \text{cm}\) and \(d_i = -12 \text{cm}\), the lens maker's formula gives us a focal length \(f\) of approximately \(3.36 \text{cm}\). This formula is critical in the design and understanding of optical systems because it directly relates the physical geometry of the lens to its optical power. Optics students must grasp this concept to understand how lenses form images and how different lens shapes affect image formation.
Object and Image Distance
The relationship between object distance (\(d_o\)) and image distance (\(d_i\)) is central to optics. Object distance is the distance from the object to the lens, whereas image distance is the distance from the image to the lens.

These distances are not arbitrary; they are governed by the lens equation \(1/f = (1/d_o) + (1/d_i)\), which provides a precise method to determine where the image will form given a certain object distance and focal length. In our example, knowing the image is \(12.0 \text{cm}\) to the left of the lens and using the magnification factor, we can determine that the object is located \(5.1 \text{cm}\) away from the lens. It is crucial to note that in lens formulas, distances on the same side as the incoming light (object side) are considered positive, while distances on the same side as the outgoing light (image side) can be negative or positive depending if the image is real or virtual. Thus, sign conventions play a role in appropriately applying these concepts. For students to solve and even predict the behavior of lenses, they must be comfortable working with these distances and understanding their impact on image formation.

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Most popular questions from this chapter

To determine the focal length \(f\) of a converging thin lens, you place a \(4.00-\mathrm{mm}\) -tall object a distance \(s\) to the left of the lens and measure the height \(h^{\prime}\) of the real image that is formed to the right of the lens. You repeat this process for several values of \(s\) that produce a real image. After graphing your results as \(1 / h^{\prime}\) versus \(s\), both in \(\mathrm{cm}\), you find that they lie close to a straight line that has slope \(0.208 \mathrm{~cm}^{-2}\). What is the focal length of the lens?

The overall angular magnification of a microscope is \(M=-178 .\) The eyepiece has focal length \(15.0 \mathrm{~mm}\) and the final image is at infinity. The separation between the two lenses is \(202 \mathrm{~mm}\). What is the focal length of the objective? Do not use the approximation \(s_{1} \approx f_{1}\) in the expression for \(M\).

The smallest object we can resolve with our eye is limited by the size of the light receptor cells in the retina. In order for us to distinguish any detail in an object, its image cannot be any smaller than a single retinal cell. Although the size depends on the type of cell (rod or cone), a diameter of a few microns \((\mu \mathrm{m})\) is typical near the center of the eye. We shall model the eye as a sphere \(2.50 \mathrm{~cm}\) in diameter with a single thin lens at the front and the retina at the rear, with light receptor cells \(5.0 \mu \mathrm{m}\) in diameter. (a) What is the smallest object you can resolve at a near point of \(25 \mathrm{~cm} ?\) (b) What angle is subtended by this object at the eye? Express your answer in units of minutes \(\left(1^{\circ}=60 \mathrm{~min}\right),\) and compare it with the typical experimental value of about \(1.0 \mathrm{~min} .\) (Note: There are other limitations, such as the bending of light as it passes through the pupil, but we shall ignore them here.)

A coin is placed next to the convex side of a thin spherical glass shell having a radius of curvature of \(18.0 \mathrm{~cm} .\) Reflection from the surface of the shell forms an image of the \(1.5-\mathrm{cm}\) -tall coin that is \(6.00 \mathrm{~cm}\) behind the glass shell. Where is the coin located? Determine the size, orientation, and nature (real or virtual) of the image.

A compound microscope has an objective lens with focal length \(14.0 \mathrm{~mm}\) and an eyepiece with focal length \(20.0 \mathrm{~mm}\). The final image is at infinity. The object to be viewed is placed \(2.0 \mathrm{~mm}\) beyond the focal point of the objective lens. (a) What is the distance between the two lenses? (b) Without making the approximation \(s_{1} \approx f_{1},\) use \(M=m_{1} M_{2}\) with \(m_{1}=-s_{1}^{\prime} / s_{1}\) to find the overall angular magnification of the microscope. (c) What is the percentage difference between your result and the result obtained if the approximation \(s_{1} \approx f_{1}\) is used to find \(M ?\)

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