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A converging lens forms an image of an 8.00-mm-tall real object. The image is 12.0 cm to the left of the lens, 3.40 cm tall, and erect. What is the focal length of the lens? Where is the object located?

Short Answer

Expert verified
The focal length is 3.69 cm, and the object is located 2.82 cm from the lens.

Step by step solution

01

Understanding the Problem

We are given an object of height 8.00 mm and an image of height 3.40 cm formed 12.0 cm to the left of the lens. The image is erect and taller than the object, indicating it's a virtual image. We must find the focal length of the lens and the object's location.
02

Convert Units for Consistency

First, convert the object height to centimeters: \(8.00 \text{ mm} = 0.80 \text{ cm}\). Now, all the measures are in centimeters.
03

Apply the Magnification Formula

The magnification \(m\) is given by the ratio of the image height \(h_i\) to the object height \(h_o\) and also by the ratio of image distance \(d_i\) to object distance \(d_o\): \[m = \frac{h_i}{h_o} = \frac{d_i}{d_o}\]. Substituting the known values: \[m = \frac{3.40 \text{ cm}}{0.80 \text{ cm}} = \frac{12.0 \text{ cm}}{d_o}\].
04

Solve for Object Distance

From \(\frac{3.40}{0.80} = \frac{12.0}{d_o}\), solve for \(d_o\): \[d_o = \frac{12.0 \text{ cm} \times 0.80 \text{ cm}}{3.40 \text{ cm}} = 2.82 \text{ cm}\].
05

Lens Formula Application

Use the lens formula \(\frac{1}{f} = \frac{1}{d_o} + \frac{1}{d_i}\). Substitute \(d_o = 2.82 \text{ cm}\) and \(d_i = -12.0 \text{ cm}\) (negative because it's a virtual image): \[\frac{1}{f} = \frac{1}{2.82} + \frac{1}{-12.0}\].
06

Calculate Focal Length

Calculate \(\frac{1}{f}\) using the values: \[\frac{1}{f} = \frac{1}{2.82} - \frac{1}{12.0} = 0.3546 - 0.0833 = 0.2713\]. Then, \(f = \frac{1}{0.2713} \approx 3.69 \text{ cm}\).

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Key Concepts

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

Magnification
Magnification is a crucial concept when dealing with optical lenses. It essentially tells us how much larger or smaller the image of an object appears, when viewed through a lens, compared to the object's actual size. To find magnification, we use the formula \( m = \frac{h_i}{h_o} \), where \( h_i \) is the image height and \( h_o \) is the object height. But that’s not all! Magnification is also related to the distances in the setup. Another equation used is \( m = \frac{d_i}{d_o} \), with \( d_i \) being the image distance and \( d_o \) the object distance. Combining these two equations allows us to solve exercises where either the height or the distances are unknown.
  • If the magnification is positive, the image is upright in relation to the object.
  • If it is negative, the image is inverted.
For instance, if the object height is less than the image height, as in our problem, we get a magnification greater than 1, indicating the image is larger than the object.
Object Distance
The object distance \( d_o \) is the distance between the object and the lens. It's an essential part of the lens formula and can be determined by rearranging the magnification formula: \( m = \frac{d_i}{d_o} \). In the solved exercise, knowing the magnification from the heights, the object distance is found by plugging in the known values. It tells us where exactly the real object is placed relative to the lens for the image to form as described. The object distance plays a pivotal role as it directly influences the size and orientation of the image.
  • For real objects (those that exist in a definite place), \( d_o \) is positive.
  • A smaller object distance generally leads to a larger image distance, significantly affecting magnification as seen in the exercise.
Image Distance
Image distance \( d_i \) is how far the image is located from the lens. The sign of \( d_i \) indicates whether an image is real or virtual. In a converging lens setup,
such as the one discussed in our exercise, the calculated image distance was -12 cm. This negative value signals that the image is virtual, and appears on the same side of the lens as the object. It is this parameter, together with object distance, that impacts image size and clarity. When applying the formula for image distance, it becomes pivotal in using the lens equation to find unknowns in the problem - especially when verified or derived from other values like focal length or magnification. Consider that:
  • A positive \( d_i \) represents a real image that appears on the opposite side of the lens from the object.
  • A negative \( d_i \) signifies a virtual image on the same side as the object, not directly visible, except through the lens.
Converging Lens
A converging lens is a type of lens that bends light rays toward a specific point, called the focal point. This kind of lens is thicker in the center than at the edges. Such lenses are commonly used in corrective glasses, projectors, and cameras. A converging lens has a specific focal length which determines where the parallel light rays meet after passing through the lens. In the context of our exercise, a focal length of approximately 3.69 cm was calculated using the lens formula: \( \frac{1}{f} = \frac{1}{d_o} + \frac{1}{d_i} \). By knowing the focal length, it's possible to predict how the lens will form an image of an object placed at various distances.
  • When the object is beyond the focal point, the lens creates a real and inverted image.
  • If the object is at the focal point, no image is formed as the rays emerge parallel.
  • When within the focal point, as seen in the exercise, a virtual, upright, and magnified image appears.

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Most popular questions from this chapter

An object is 16.0 cm to the left of a lens. The lens forms an image 36.0 cm to the right of the lens. (a) What is the focal length of the lens? Is the lens converging or diverging? (b) If the object is 8.00 mm tall, how tall is the image? Is it erect or inverted? (c) Draw a principal-ray diagram.

The cornea behaves as a thin lens of focal length approximately 1.8 cm, although this varies a bit. The material of which it is made has an index of refraction of 1.38, and its front surface is convex, with a radius of curvature of 5.0 mm. (a) If this focal length is in air, what is the radius of curvature of the back side of the cornea? (b) The closest distance at which a typical person can focus on an object (called the near point) is about 25 cm, although this varies considerably with age. Where would the cornea focus the image of an 8.0-mm-tall object at the near point? (c) What is the height of the image in part (b)? Is this image real or virtual? Is it erect or inverted? (\(Note:\) The results obtained here are not strictly accurate because, on one side, the cornea has a fluid with a refractive index different from that of air.)

A person swimming 0.80 m below the surface of the water in a swimming pool looks at the diving board that is directly overhead and sees the image of the board that is formed by refraction at the surface of the water. This image is a height of 5.20 m above the swimmer. What is the actual height of the diving board above the surface of the water?

In a simplified model of the human eye, the aqueous and vitreous humors and the lens all have a refractive index of 1.40, and all the bending occurs at the cornea, whose vertex is 2.60 cm from the retina. What should be the radius of curvature of the cornea such that the image of an object 40.0 cm from the cornea's vertex is focused on the retina?

You hold a spherical salad bowl 60 cm in front of your face with the bottom of the bowl facing you. The bowl is made of polished metal with a 35 cm radius of curvature. (a) Where is the image of your 5.0 cm tall nose located? (b) What are the image's size, orientation, and nature (real or virtual)?

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