Problem 44
Question
A concave lens of focal length \(20 \mathrm{~cm}\) produces an image half in size of the real object. The distance of the real object is (a) \(20 \mathrm{~cm}\) (b) \(30 \mathrm{~cm}\) (c) \(10 \mathrm{~cm}\) (d) \(60 \mathrm{~cm}\)
Step-by-Step Solution
Verified Answer
The distance of the real object is 60 cm.
1Step 1: Understand the Lens Formula
The lens formula is given by \( \frac{1}{f} = \frac{1}{v} - \frac{1}{u} \), where \( f \) is the focal length, \( v \) is the image distance, and \( u \) is the object distance. For a concave lens, the focal length \( f \) is negative.
2Step 2: Identify Conditions for the Problem
Given that the image is half the size of the object, the magnification \( m \) is -0.5 (negative because the image is virtual and upright in a concave lens). Remember, \( m = \frac{v}{u} \), so we have \( -0.5 = \frac{v}{u} \), or \( v = -0.5u \).
3Step 3: Substitute Known Values
We are given \( f = -20 \text{ cm} \) and from Step 2, \( v = -0.5u \). We substitute these into the lens formula: \( \frac{1}{-20} = \frac{1}{-0.5u} - \frac{1}{u} \).
4Step 4: Solve the Equation for Object Distance
Rearrange and solve the equation: \[-\frac{1}{20} = -\frac{2}{u} - \frac{1}{u}\] \[-\frac{1}{20} = -\frac{3}{u}\] and thus, \( u = 60 \text{ cm} \).
5Step 5: Confirm with the Set of Choices
Compare \( u = 60 \text{ cm} \) with the given options: (a) 20 cm, (b) 30 cm, (c) 10 cm, (d) 60 cm. Option (d) is correct.
Key Concepts
Lens FormulaFocal LengthMagnification
Lens Formula
The lens formula is a fundamental equation used to relate the focal length of a lens with the object and image distances. It is expressed as:\[ \frac{1}{f} = \frac{1}{v} - \frac{1}{u} \]Here,
- f is the focal length of the lens.
- v is the image distance from the lens.
- u is the object distance from the lens.
- Distances measured in the same direction as the incident light are positive.
- Distances against the direction of the light are negative.
- Focal lengths for concave lenses are negative.
Focal Length
The focal length is a crucial parameter of a lens, denoting the distance from the lens to the point where rays converge to form an image. For a concave lens, the focal length (
f) is negative, indicating that it does not converge light but instead makes it diverge. This divergence gives an impression that the light is originating from a point on the same side of the lens as the object, outside the lens.
Key Characteristics of Focal Length
- Concave lenses are also known as diverging lenses because of their ability to spread out incoming light rays.
- The focal point, shown virtually on the same side as the light source, indicates the illusionary origin of light after passing through the lens.
- The shorter the focal length, the stronger the diverging power of the lens.
Magnification
Magnification is a measure of how much larger or smaller an image is compared to the object itself. For lenses, magnification (m) is calculated using:\[ m = \frac{v}{u} \]Here,
- v is the image distance.
- u is the object distance.
Important Points about Magnification
- A negative magnification value implies an upright and virtual image.
- In concave lenses, magnification values range between 0 and -1, indicating diminished image sizes.
- This helps predict not only how much smaller the image appears but also confirms the virtual nature of the image produced by concave lenses.
Other exercises in this chapter
Problem 42
The length of the compound microscope is \(14 \mathrm{~cm}\). The magnifying power for relaxed eye is \(25 .\) If the focal length of eyelens is \(5 \mathrm{~cm
View solution Problem 43
A convex lens of foeal length \(f\) produces a virtual image \(n\) times the size of the object. Then the distance of the object from the lens is (a) \((n-1) f\
View solution Problem 44
An object is kept at a distance of \(16 \mathrm{~cm}\) from a thin lens and the image formed is real. If the object is kept at a distance of \(6 \mathrm{~cm}\)
View solution Problem 45
An object \(15 \mathrm{~cm}\) high is placed \(10 \mathrm{~cm}\) from the optical centre of a thin lens. Its image is formed \(25 \mathrm{~cm}\) from the optica
View solution