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Determine the nature, position, and transverse magnification of the image formed by a thin converging lens of focal length \(+100 \mathrm{~cm}\) when the object distance from the lens is \((a) 150 \mathrm{~cm},(b) 75.0 \mathrm{~cm}\).

Short Answer

Expert verified
For (a), the image is real, inverted at 300 cm; magnification is -2. For (b), the image is virtual, upright at -300 cm; magnification is 4.

Step by step solution

01

Understanding the Lens Formula

To solve the problem, we need to use the lens formula: \(\frac{1}{f} = \frac{1}{d_o} + \frac{1}{d_i}\), where \(f\) is the focal length of the lens, \(d_o\) is the object distance, and \(d_i\) is the image distance. Here, \(f = +100 \text{ cm}\).
02

Case (a): Finding Image Distance for \(d_o = 150\text{ cm}\)

Substitute \(f = +100\text{ cm}\) and \(d_o = 150\text{ cm}\) into the lens formula: \[ \frac{1}{100} = \frac{1}{150} + \frac{1}{d_i} \]. Solve for \(d_i\): \[ \frac{1}{d_i} = \frac{1}{100} - \frac{1}{150} = \frac{3-2}{300} = \frac{1}{300} \]. Therefore, \(d_i = 300 \text{ cm}\).
03

Calculating Magnification for Case (a)

The transverse magnification \(m\) is given by \(m = -\frac{d_i}{d_o}\). For \(d_i = 300\text{ cm}\) and \(d_o = 150\text{ cm}\): \[ m = -\frac{300}{150} = -2 \].
04

Assessing Nature of Image for Case (a)

Since \(d_i\) is positive, the image is real and located on the opposite side of the object. The negative magnification indicates the image is inverted.
05

Case (b): Finding Image Distance for \(d_o = 75 \text{ cm}\)

Substitute \(f = +100\text{ cm}\) and \(d_o = 75\text{ cm}\) into the lens formula: \[ \frac{1}{100} = \frac{1}{75} + \frac{1}{d_i} \]. Solve for \(d_i\): \[ \frac{1}{d_i} = \frac{1}{100} - \frac{1}{75} = \frac{3-4}{300} = -\frac{1}{300} \]. Therefore, \(d_i = -300 \text{ cm}\).
06

Calculating Magnification for Case (b)

For \(d_i = -300\text{ cm}\) and \(d_o = 75\text{ cm}\): \[ m = -\frac{-300}{75} = 4 \].
07

Assessing Nature of Image for Case (b)

Since \(d_i\) is negative, the image is virtual and located on the same side as the object. The positive magnification means the image is upright.

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Key Concepts

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

Lens Formula
The lens formula is a crucial tool for understanding how light interacts with lenses. It relates the object distance, image distance, and focal length of the lens. This formula is expressed as:\[ \frac{1}{f} = \frac{1}{d_o} + \frac{1}{d_i} \]Here, \(f\) is the focal length (positive for converging lenses), \(d_o\) is the distance from the object to the lens, and \(d_i\) is the distance from the image to the lens. The lens formula helps determine the position of the image formed by a lens when the object distance and focal length are known.
In our exercise, understanding the lens formula is the first step in finding the image distance for a converging lens. By rearranging and solving, we can calculate \(d_i\), the position where the image forms, which is critical for determining the nature of the image.
Image Distance
Image distance, denoted as \(d_i\), describes how far the formed image is from the lens. When solving optical problems with lenses, determining \(d_i\) gives insight into the physical layout of the imaging system.
For a converging lens:
  • If \(d_i\) is positive, the image forms on the opposite side of the object, signifying a real image.
  • If \(d_i\) is negative, the image appears on the same side as the object, indicating a virtual image.

In our specific exercise:- With an object distance \(d_o = 150\text{ cm}\), \(d_i = 300\text{ cm}\), showing a real image.- For \(d_o = 75\text{ cm}\), \(d_i = -300\text{ cm}\), demonstrating a virtual image.
This essential measurement helps classify the type and orientation of the image.
Transverse Magnification
Transverse magnification (\(m\)) describes how much larger or smaller the image is compared to the object. It is defined mathematically as the ratio of the image distance to the object distance, with a negative sign:\[ m = -\frac{d_i}{d_o} \]The sign of \(m\) provides additional insights:
  • A negative magnification indicates that the image is inverted compared to the object.
  • A positive magnification suggests that the image is upright.

For the given exercise:- Case (a): With a magnification of \(-2\), the image is inverted and twice the size of the object.- Case (b): With a magnification of \(4\), the image is upright and four times larger than the object.
Understanding magnification is essential for predicting how the image will appear in relation to the original object.
Real and Virtual Images
A lens can form images that are either real or virtual, two distinct types each with its characteristics.
**Real Images:**
  • Form on the opposite side of the lens from the object.
  • Can be projected onto a screen.
  • Typically inverted from the object.
**Virtual Images:**
  • Appear on the same side as the object relative to the lens.
  • Cannot be projected; only visible when looking through the lens.
  • Generally upright.

In the specific cases of our exercise:- When the object is placed at \(150\text{ cm}\) from the lens, a real image is formed at \(300\text{ cm}\) on the opposite side.- At an object distance of \(75\text{ cm}\), a virtual image appears at \(-300\text{ cm}\) on the same side.
Knowing whether an image is real or virtual is important in applications ranging from everyday lenses like eyeglasses to complex optical instruments.

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Most popular questions from this chapter

What are the nature and focal length of the thin lens that will form a real image having one-third the dimensions of an object located \(9.0 \mathrm{~cm}\) from the lens?

Compute the focal length of a lens which will give an erect image \(10 \mathrm{~cm}\) from the lens when the object distance from the lens is ( \(a\) ) \(200 \mathrm{~cm},(b)\) very great.

Two thin lenses, of focal lengths \(+9.0\) and \(-6.0 \mathrm{~cm}\), are placed in contact. Calculate the focal length of the combination. $$ \frac{1}{f}=\frac{1}{f_{1}}+\frac{1}{f_{2}}=\frac{1}{9.0 \mathrm{~cm}}-\frac{1}{6.0 \mathrm{~cm}}=-\frac{1}{18 \mathrm{~cm}} \quad \text { or } \quad f=-18 \mathrm{~cm} $$ The combination lens is diverging.

A double convex thin lens has radii of \(20.0 \mathrm{~cm}\). The index of refraction of the glass is 1.50. Compute the focal length of this lens \((a)\) in air and \((b)\) when it is immersed in carbon disulfide \((n=1.63)\). For a thin lens with an index of \(n_{1}\), immersed in a surrounding medium of index \(n_{2}\), $$ \frac{1}{f}=\left(\frac{n_{1}}{n_{2}}-1\right)\left(\frac{1}{R_{1}}-\frac{1}{R_{2}}\right) $$ Here \(R_{1}=+20.0 \mathrm{~cm}\) and \(R_{2}=-20.0 \mathrm{~cm}\) and so (a) \(\frac{1}{f}=(1.50-1)\left(\frac{1}{20 \mathrm{~cm}}-\frac{1}{-20 \mathrm{~cm}}\right) \quad\) or \(\quad f=+20.0 \mathrm{~cm}\) (b) \(\frac{1}{f}=\left(\frac{1.50}{1.63}-1\right)\left(\frac{1}{20 \mathrm{~cm}}-\frac{1}{-20 \mathrm{~cm}}\right) \quad\) or \(\quad f=-125 \mathrm{~cm}\) When \(n_{2}>n_{1}\) the focal length is negative and the lens is a diverging lens.

A thin glass lens \((n=1.50)\) has a focal length of \(+10 \mathrm{~cm}\) in air. Compute its focal length in water \((n=1.33)\). Using $$ \frac{1}{f}=\left(\frac{n_{1}}{n_{2}}-1\right)\left(\frac{1}{R_{1}}-\frac{1}{R_{2}}\right) $$ we get For air: \(\quad \frac{1}{10}=(1.50-1)\left(\frac{1}{R_{1}}-\frac{1}{R_{2}}\right)\) $$ \text { \mathrm{\\{} F o r ~ w a t e r : ~ } \quad \frac{1}{f}=\left(\frac{1.50}{1.33}-1\right)\left(\frac{1}{R_{1}}-\frac{1}{R_{2}}\right) $$ Divide one equation by the other to obtain \(f=5.0 / 0.128=39 \mathrm{~cm}\).

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