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A short linear object of length \(L\) lies on the axis of a spherical mirror of focal length of \(f\) at a distance \(u\) from the mirror. Its image has an axial length \(L^{\prime}\) equal to \(\ldots \ldots \ldots\).. (A) \(\mathrm{L}[\mathrm{f} /(\mathrm{u}-\mathrm{f})]^{2}\) (B) \(\mathrm{L}[(\mathrm{u}-\mathrm{f}) / \mathrm{f}]^{2}\) (C) \(\mathrm{L}[(\mathrm{u}+\mathrm{f}) / \mathrm{f}]^{1 / 2}\) (D) \(L[f /(u-f)]^{1 / 2}\)

Short Answer

Expert verified
The short answer for the image's axial length \(L'\) is: \(L' = L\frac{f}{u - f}\)

Step by step solution

01

Understand the question

We are given a linear object of length L, placed on the axis of a spherical mirror with focal length f and object distance u. We are asked to find the image length L'. Write the lens/mirror equation and magnification formula to relate these values: Lens/mirror equation: \[\frac{1}{f} = \frac{1}{u} + \frac{1}{v}\] Magnification formula: \[m = \frac{L'}{L} = -\frac{v}{u}\] #Step 2: Express v in terms of u, f, and L#
02

Solve for image distance v

Rearrange the lens/mirror equation to express v in terms of u and f: \[\frac{1}{v} = \frac{1}{f} - \frac{1}{u}\] \[v = \frac{uf}{u - f}\] #Step 3: Plug v into the magnification formula and solve for L'#
03

Plug v into magnification formula

Substitute the expression for v from step 2 into the magnification formula: \[-\frac{L'}{L} = \frac{uf}{u(u - f)}\] #Step 4: Solve for L'#
04

Solve for image length L'

Isolate L' to find an expression for the image length: \[L' = -L \frac{uf}{u(u - f)}\] Since the magnification formula's negative sign indicates the image is inverted, remove the negative sign for the image length as we are only interested in the axial length L': \[L' = L\frac{uf}{u(u - f)}\] Now, simplify the expression for L': \[L' = L\frac{f}{u - f}\] Squaring both sides, we get: \[{L'}^2 = L^2\left[\frac{f}{u - f}\right]^2\] Comparing this with the given options, the correct answer is: (A) \(\mathrm{L}[\mathrm{f} /(\mathrm{u}-\mathrm{f})]^{2}\)

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Most popular questions from this chapter

The distance between object and the screen is D. Real images of an object are formed on the screen two positions of a lens separated by a distance \(\mathrm{d}\). What will be the ratio between the sizes of two images? (A) \(\left(\mathrm{D}^{2} / \mathrm{d}^{2}\right)\) (B) \((\mathrm{D} / \mathrm{d})\) (C) \(\sqrt{(\mathrm{D} / \mathrm{d})}\) (D) \(\left[(\mathrm{D}-\mathrm{d})^{2} /(\mathrm{D}+\mathrm{d})^{2}\right]\)

A thin lens has focal length \(\mathrm{f}\), and its aperture has diameter d. It forms an image of intensity I. Now, the central part of the aperture upto diameter \((\mathrm{d} / 2)\) is blocked by an opaque paper. The focal length and image intensity will change to \(\ldots\) (A) \(\mathrm{f}\) and \((3 \mathrm{I} / 4)\) (B) \((3 \mathrm{f} / 4)\) and \((\mathrm{I} / 2)\) (C) \(\mathrm{f}\) and \((\mathrm{I} / 4)\) (D) \((\mathrm{f} / 2)\) and \((\mathrm{I} / 2)\)

An object is placed at a distance of \((\mathrm{f} / 2)\) the from a convex lens the image will be.... (A) at \(\mathrm{f}\), real and inverted (B) at,\((3 \mathrm{f} / 2)\) real and inverted (C) at one of the foci, virtual and double its size (D) at \(2 \mathrm{f}\), virtual and erect.

A concave lens of focal length \(\mathrm{f}\) forms an image which is n times the size of the object. What is the distance of the object from the lens? (A) \((1+\mathrm{n}) \mathrm{f}\) (B) \((1-\mathrm{n}) \mathrm{f}\) (C) \([(1-\mathrm{n}) / \mathrm{n}] \mathrm{f}\) (D) \([(1+\mathrm{n}) / \mathrm{n}] \mathrm{f}\)

A concave mirror of focal length \(\mathrm{f}\) produces an images n times the size of the object. If the image is real then What is the distance of the object from the mirror? (A) \((\mathrm{n}+1) \mathrm{f}\) (B) \([(\mathrm{n}-1) / \mathrm{n}] \mathrm{f}\) (C) \((\mathrm{n}-1) \mathrm{f}\) (D) \([(\mathrm{n}+1) / \mathrm{n}] \mathrm{f}\)

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