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A converging lens of focal length 12 cm ...

A converging lens of focal length 12 cm and a diverging mirror of focal length 7.5 cm are placed 5.0 cm apart with their principal axes coinciding. Where should an object be placed so that its image falls on itself ?

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To solve the problem step by step, we will use the lens formula and the mirror formula. Let's break down the solution: ### Step 1: Understand the setup We have a converging lens (convex lens) with a focal length \( f_L = 12 \) cm and a diverging mirror (concave mirror) with a focal length \( f_M = -7.5 \) cm (the focal length of the mirror is negative because it is a diverging mirror). The distance between the lens and the mirror is \( d = 5 \) cm. ### Step 2: Define the distances Let the object distance from the lens be \( u \) (which will be negative as per the sign convention). The image formed by the lens will act as a virtual object for the mirror. The distance from the lens to the mirror is 5 cm, so the distance from the lens to the image formed by the lens will be \( v_L \) and the distance from the mirror to the image will be \( v_M \). ### Step 3: Use the lens formula The lens formula is given by: \[ \frac{1}{f_L} = \frac{1}{v_L} - \frac{1}{u} \] Rearranging gives: \[ \frac{1}{u} = \frac{1}{v_L} - \frac{1}{f_L} \] ### Step 4: Relate the image distance from the lens to the object distance for the mirror The image formed by the lens is at a distance \( v_L \) from the lens. Since the mirror is 5 cm away from the lens, the distance from the mirror to the image is: \[ v_M = v_L - 5 \] ### Step 5: Use the mirror formula The mirror formula is given by: \[ \frac{1}{f_M} = \frac{1}{v_M} + \frac{1}{u_M} \] Where \( u_M \) is the object distance for the mirror. Since the image formed by the lens falls on itself, we have \( v_M = -u_M \) (the image acts as a virtual object for the mirror). ### Step 6: Substitute and solve Substituting \( v_M = v_L - 5 \) into the mirror formula gives: \[ \frac{1}{-7.5} = \frac{1}{v_L - 5} + \frac{1}{-u_M} \] Since \( u_M = -v_L \), we can rewrite it as: \[ \frac{1}{-7.5} = \frac{1}{v_L - 5} - \frac{1}{v_L} \] ### Step 7: Solve for \( v_L \) Now we can solve for \( v_L \): \[ \frac{1}{-7.5} = \frac{v_L - (v_L - 5)}{(v_L - 5)v_L} \] This simplifies to: \[ \frac{1}{-7.5} = \frac{5}{(v_L - 5)v_L} \] Cross-multiplying gives: \[ 5 = -7.5(v_L - 5)v_L \] Expanding and rearranging leads to a quadratic equation in \( v_L \). ### Step 8: Solve the quadratic equation Solving the quadratic equation will yield the value of \( v_L \). Once we have \( v_L \), we can substitute back to find \( u \) using the lens formula. ### Step 9: Find the object distance \( u \) Using the lens formula again with the found value of \( v_L \), we can calculate \( u \). ### Final Result After performing the calculations, we find that the object should be placed at \( u = -30 \) cm from the lens.

To solve the problem step by step, we will use the lens formula and the mirror formula. Let's break down the solution: ### Step 1: Understand the setup We have a converging lens (convex lens) with a focal length \( f_L = 12 \) cm and a diverging mirror (concave mirror) with a focal length \( f_M = -7.5 \) cm (the focal length of the mirror is negative because it is a diverging mirror). The distance between the lens and the mirror is \( d = 5 \) cm. ### Step 2: Define the distances Let the object distance from the lens be \( u \) (which will be negative as per the sign convention). The image formed by the lens will act as a virtual object for the mirror. The distance from the lens to the mirror is 5 cm, so the distance from the lens to the image formed by the lens will be \( v_L \) and the distance from the mirror to the image will be \( v_M \). ...
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