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A converging lens with a focal length of \(12.0 \mathrm{~cm}\) forms a virtual image \(8.00 \mathrm{~mm}\) tall, \(17.0 \mathrm{~cm}\) to the right of the lens. Determine the position and size of the object. Is the image erect or inverted? Are the object and image on the same side or opposite sides of the lens? Draw a principal-ray diagram for this situation.

Short Answer

Expert verified
The object distance and height are calculated using the lens and magnification equations. The image is inverted and exists on the opposite side of the lens from where the object is placed.

Step by step solution

01

STEP 1: Lens Equation

First, use the lens equation: \(1/f = 1/d_o + 1/d_i\), where \(f\) is the focal length, \(d_o\) is the object distance, and \(d_i\) is the distance to the image. Here, \(f = 12.0cm\) and \(d_i = 17.0cm\). Solve this equation for \(d_o\)\.
02

STEP 2: Solve for Object Distance

Plug in the known values into the lens equation: \(1/12.0 = 1/d_o + 1/17.0\). To solve for \(d_o\), rewrite the equation to \(1/d_o = 1/12.0 - 1/17.0\) and calculate \(d_o\).
03

STEP 3: Magnification Equation

Now use the magnification equation: \(m = -d_i / d_o = h_i / h_o\), where \(m\) is the magnification factor, \(h_i\) is the image height and \(h_o\) is the object height.
04

STEP 4: Solve for Object Height

Insert the known values and the computed \(d_o\) into the magnification equation: \(-17.0 / d_o = 8.0 / h_o\). Solve for \(h_o\).
05

STEP 5: Image Orientation and Position

Since the image distance \(d_i\) is positive, the image is on the opposite side of the lens from where the object is placed, according to the sign convention for lenses. The magnification factor is negative, which means the image is inverted.

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Key Concepts

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

Lens Equation
The lens equation is a fundamental principle used to determine the relationship between the object distance (\(d_o\)), the image distance (\(d_i\)), and the focal length (\f) of a converging lens. This equation is given as 1/f = 1/d_o + 1/d_i.
The equation helps us calculate any one of these variables if the others are known. A positive image distance indicates a real image formed on the opposite side of the lens from the object. However, if the value for image distance is negative, it describes a virtual image located on the same side as the object. This equation is essential to identifying how the image will be formed through the lens. In our exercise, applying the lens equation permitted us to find the object distance, ultimately leading to further insights about our image, such as size and position.
Object Distance
Object distance, denoted as d_o,
refers to the distance between the object and the lens in optics. It plays a critical role in image formation and directly influences the size and nature of the image produced. Object distance is a variable in the lens equation, and understanding its value is necessary for predicting whether an image will be real or virtual, erect or inverted. A real, inverted image is formed when the object is placed outside the focal point of a converging lens. In contrast, when an object is within the focal length, a virtual, erect image is formed. By calculating the object distance in our example, students can deduce the characteristics and orientation of an image formed by a lens.
Image Distance
In contrast to object distance, image distance (d_i)
is the distance from the lens to the image it forms. Similar to object distance, this variable in the lens equation helps determine the characteristics of the resultant image. In the example, the positive value of the image distance indicates that a real image is produced. However, when dealing with virtual images, the value of d_i
is taken as negative. It's important to note that image distance is also closely related to the concept of magnification; a larger absolute value of d_i
typically means a larger image when compared to the size of the object. Image distance gives us a concrete measure to predict where the image will form and assists us in drawing accurate ray diagrams.
Magnification in Optics
Magnification is a measure that tells us how much larger or smaller the image is when compared to the object itself. The magnification equation is m = -d_i / d_o = h_i / h_o,
where m
is the magnification factor, h_i
is the height of the image, and h_o
is the height of the object. A magnification value of 1 means the image is the same size as the object. If the magnification is negative, as it is in our example, the image is inverted relative to the object. When the value of magnification is greater than 1, the image is enlarged; conversely, if it is less than 1, the image is reduced in size.
Ray Diagrams
Ray diagrams are visual tools used in optics to illustrate the path light rays take as they pass through lenses. These diagrams help us to understand how images are formed and to describe their properties, such as position, size, and orientation. To draw a ray diagram, you generally plot at least two of the principal rays: one ray that passes through the center of the lens undeviated, and another that passes parallel to the principal axis and then through the focal point on the other side of the lens. In our textbook example, a ray diagram would show that the image is both inverted and formed on the opposite side of the lens from the object. Ray diagrams are not only an essential tool in understanding lenses, but they are also a key element in explaining the theoretical background in optical systems and in demonstrating the principles discussed in the lens equation, object distance, image distance, and magnification.

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Most popular questions from this chapter

A person is lying on a diving board \(3.00 \mathrm{~m}\) above the surface of the water in a swimming pool. She looks at a penny that is on the bottom of the pool directly below her. To her, the penny appears to be a distance of \(7.00 \mathrm{~m}\) from her. What is the depth of the water at this point?

A mirror on the passenger side of your car is convex and has a radius of curvature with magnitude \(18.0 \mathrm{~cm} .\) (a) Another car is behind your car, \(9.00 \mathrm{~m}\) from the mirror, and this car is viewed in the mirror by your passenger. If this car is \(1.5 \mathrm{~m}\) tall, what is the height of the image? (b) The mirror has a warning attached that objects viewed in it are closer than they appear. Why is this so?

The cornea of the eye has a radius of curvature of approximately \(0.50 \mathrm{~cm},\) and the aqueous humor behind it has an index of refraction of \(1.35 .\) The thickness of the cornea itself is small enough that we shall neglect it. The depth of a typical human eye is around \(25 \mathrm{~mm}\). (a) What would have to be the radius of curvature of the cornea so that it alone would focus the image of a distant mountain on the retina, which is at the back of the eye opposite the cornea? (b) If the cornea focused the mountain correctly on the retina as described in part (a), would it also focus the text from a computer screen on the retina if that screen were \(25 \mathrm{~cm}\) in front of the eye? If not, where would it focus that text: in front of or behind the retina? (c) Given that the cornea has a radius of curvature of about \(5.0 \mathrm{~mm}\), where does it actually focus the mountain? Is this in front of or behind the retina? Does this help you see why the eye needs help from a lens to complete the task of focusing?

It is your first day at work as a summer intern at an optics company. Your supervisor hands you a diverging lens and asks you to measure its focal length. You know that with a converging lens, you can measure the focal length by placing an object a distance \(s\) to the left of the lens, far enough from the lens for the image to be real, and viewing the image on a screen that is to the right of the lens. By adjusting the position of the screen until the image is in sharp focus, you can determine the image distance \(s^{\prime}\) and then use Eq. (34.16) to calculate the focal length \(f\) of the lens. But this procedure won't work with a diverging lens - by itself, a diverging lens produces only virtual images, which can't be projected onto a screen. Therefore, to determine the focal length of a diverging lens, you do the following: First you take a converging lens and measure that, for an object \(20.0 \mathrm{~cm}\) to the left of the lens, the image is \(29.7 \mathrm{~cm}\) to the right of the lens. You then place a diverging lens \(20.0 \mathrm{~cm}\) to the right of the converging lens and measure the final image to be \(42.8 \mathrm{~cm}\) to the right of the converging lens. Suspecting some inaccuracy in measurement, you repeat the lenscombination measurement with the same object distance for the converging lens but with the diverging lens \(25.0 \mathrm{~cm}\) to the right of the converging lens. You measure the final image to be \(31.6 \mathrm{~cm}\) to the right of the converging lens. (a) Use both lens-combination measurements to calculate the focal length of the diverging lens. Take as your best experimental value for the focal length the average of the two values. (b) Which position of the diverging lens, \(20.0 \mathrm{~cm}\) to the right or \(25.0 \mathrm{~cm}\) to the right of the converging lens, gives the tallest image?

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.

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