/*! 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 0 (II) A lighted candle is placed ... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

(II) A lighted candle is placed 36 \(\mathrm{cm}\) in front of a converging lens of focal length \(f_{1}=13 \mathrm{cm},\) which in turn is 56 \(\mathrm{cm}\) in front of another converging lens of focal length \(f_{2}=16 \mathrm{cm}\) (see Fig. \(47 ) .(a)\) Draw a ray diagram and estimate the location and the relative size of the final image. (b) Calculate the position and relative size of the final image.

Short Answer

Expert verified
Final image is 29.07 cm from the second lens, size is 46.2% of original.

Step by step solution

01

Analyze the First Lens

For the first lens with focal length \(f_1 = 13\, \text{cm}\), use the lens equation: \(\frac{1}{f_1} = \frac{1}{d_{o1}} + \frac{1}{d_{i1}}\), where \(d_{o1} = 36\, \text{cm}\) is the object distance.Solving for \(d_{i1}\), the image distance:\[\frac{1}{d_{i1}} = \frac{1}{f_1} - \frac{1}{d_{o1}} = \frac{1}{13} - \frac{1}{36}\]\[\frac{1}{d_{i1}} = \frac{36 - 13}{13 \times 36} = \frac{23}{468} \approx 0.0491\]\[d_{i1} = \frac{1}{0.0491} \approx 20.37\, \text{cm}\]Thus, the image formed by the first lens is approximately \(20.37\, \text{cm}\) from it.
02

Locate the Image as the Object for the Second Lens

The image formed by the first lens acts as a virtual object for the second lens.Since the lenses are \(56\, \text{cm}\) apart, the distance from the second lens to the image from the first lens \(d_{o2}\) is:\[d_{o2} = 56 - d_{i1} = 56 - 20.37 = 35.63\, \text{cm}\]
03

Analyze the Second Lens

Now use the lens equation for the second lens with \(f_2 = 16\, \text{cm}\):\[\frac{1}{f_2} = \frac{1}{d_{o2}} + \frac{1}{d_{i2}}\] Solving for \(d_{i2}\), the final image distance:\[\frac{1}{d_{i2}} = \frac{1}{f_2} - \frac{1}{d_{o2}} = \frac{1}{16} - \frac{1}{35.63}\]\[\frac{1}{d_{i2}} = \frac{35.63 - 16}{35.63 \times 16}\approx \frac{19.63}{570.08} \approx 0.0344\]\[d_{i2} = \frac{1}{0.0344} \approx 29.07\, \text{cm}\]The final image is \(29.07 \text{ cm}\) on the other side of the second lens.
04

Calculate the Magnification

The magnification for each lens is given by the formula \(m = -\frac{d_i}{d_o}\). For the first lens:\[m_1 = -\frac{d_{i1}}{d_{o1}} = -\frac{20.37}{36} \approx -0.566\]For the second lens:\[m_2 = -\frac{d_{i2}}{d_{o2}} = -\frac{29.07}{35.63} \approx -0.816\]The total magnification is the product of the two:\[m_{total} = m_1 \times m_2 = (-0.566) \times (-0.816) \approx 0.462\]
05

Conclusion

The final image is located approximately \(29.07 \text{ cm}\) on the opposite side of the second lens relative to the image formed by the first lens. The image size is approximately \(46.2\%\) of the original object size, and it is upright with respect to the original object.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

Key Concepts

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

Understanding Converging Lenses
A converging lens, often called a convex lens, bends light rays such that they come together or "converge" to a point called the focal point. These lenses are thicker in the middle than at the edges, and this unique shape is what helps to converge light. When an object is placed in front of a converging lens, it creates an image.
To understand how an image forms, let's look at two main components: the focal length and the object distance. The focal length is the distance from the center of the lens to the focal point, and it’s a crucial part of the lens equation. In a converging lens, the focal length is positive, which means it converges light to a real point on the opposite side of the lens from the object.
In our exercise, we have two converging lenses with focal lengths of 13 cm and 16 cm respectively. Using the lens equation, \(\frac{1}{f} = \frac{1}{d_o} + \frac{1}{d_i}\), where \(f\) is the focal length, \(d_o\) is the object distance, and \(d_i\) is the image distance, helps determine where each lens will form its image. This methodical approach is essential for correctly predicting the behavior of lenses in optical systems.
Calculating Image Distance
Image distance refers to the distance between the lens and the image it forms. This is a critical measurement because it helps determine where the image will appear and its properties.
For a converging lens, if an object is placed beyond the focal length, the ray diagrams and lens equation allow us to find the image distance. This is represented in the equation \(\frac{1}{f} = \frac{1}{d_o} + \frac{1}{d_i}\). This formula is used to solve for \(d_i\), the image distance. It works because it relates the focal length of the lens and the object distance to the resulting image distance.
In the original exercise, the first lens has an object placed at 36 cm in front of it, resulting in an image distance of around 20.37 cm calculated using the lens formula. This image then acts as a virtual object for the second lens, allowing its position to be worked out similarly. The combination of these distances determines the final image position relative to the original object, as seen with the second lens calculation to find an image distance of approximately 29.07 cm.
Exploring Magnification
Magnification tells us how much larger or smaller the image is compared to the actual object. It’s determined by the formula \(m = -\frac{d_i}{d_o}\), where \(d_i\) is the image distance and \(d_o\) is the object distance. The negative sign indicates that the image formed by a single lens is inverted.
For example, in our exercise, the first lens has a calculated magnification of around -0.566, indicating that the image is smaller than the object and inverted. The second lens has a further effect, altering the magnification to approximately -0.816. The overall magnification of the system is the product of the individual magnifications, resulting in an image that is about 46.2% the size of the original object and upright, since multiplying two negative magnifications results in a positive product.
Understanding magnification is crucial, especially in devices like microscopes and cameras, where accurate size representation is key. Whether enlarging or reducing the size of an image significantly impacts how we interpret the visual information.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

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 \(25 \mathrm{~cm} ?\)

(II) What is the focal length of the eye lens system when viewing an object (a) at infinity, and (b) \(38 \mathrm{~cm}\) from the eye? Assume that the lens- retina distance is \(2.0 \mathrm{~cm}\).

A telephoto lens system obtains a large magnification in a compact package. A simple such system can be constructed out of two lenses, one converging and one diverging, of focal lengths \(f_{1}\) and \(f_{2}=-\frac{1}{2} f_{1},\) respectively, separated by a distance \(\ell=\frac{3}{4} f_{1}\) as shown in Fig. \(51 .\) (a) For a distant object located at distance \(d_{\mathrm{o}}\) from the first lens, show that the first lens forms an image with magnification \(m_{1} \approx-f_{1} / d_{0}\) located very close to its focal point. Go on to show that the total magnification for the two-lens system is \(m \approx-2 f_{1} / d_{0} .(b)\) For an object located at infinity, show that the two-lens system forms an image that is a distance \(\frac{5}{4} f_{1}\) behind the first lens. (c) A single 250 -mm-focal-length lens would have to be mounted about 250 \(\mathrm{mm}\) from a camera's film in order to produce an image of a distant object at \(d_{\mathrm{o}}\) with magnification \(-(250 \mathrm{mm}) / d_{\mathrm{o}} .\) To produce an image of this object with the same magnification using the two-lens system, what value of \(f_{1}\) should be used and how far in front of the film should the first lens be placed? How much smaller is the "focusing length" (i.e., first lens-to-final image distance) of this two-lens system in comparison with the \(250-\mathrm{mm}\) "focusing length" of the equivalent single lens?

(I) What is the magnification of an astronomical telescope whose objective lens has a focal length of \(78 \mathrm{~cm}\), and whose eyepiece has a focal length of \(2.8 \mathrm{~cm} ?\) What is the overall length of the telescope when adjusted for a relaxed eye?

(a) Show that if two thin lenses of focal lengths \(f_{1}\) and \(f_{2}\) are placed in contact with each other, the focal length of the combination is given by \(f_{\mathrm{T}}=f_{1} f_{2} /\left(f_{1}+f_{2}\right)\). (b) Show that the power \(P\) of the combination of two lenses is the sum of their separate powers, \(P=P_{1}+P_{2}\)

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.