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Focal length of a lens in air is f. Refr...

Focal length of a lens in air is f. Refractive index of the lens is `mu`. Focal length changes to `f_(1)` if lens is immersed in a liquid of refractive index `(mu)/(2)` and it becomes `f_(2)` if the lens is immersed in a liquid of refractive index `2 mu`. Then

A

`f_(1) = (f)/(2)`

B

`f_(2) = -2f`

C

`f_(2) = -(3f)/(2)`

D

Data is insufficient

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we will use the lens maker's formula, which relates the focal length of a lens to the refractive indices of the lens and the surrounding medium. The formula is given by: \[ \frac{1}{f} = \left( \frac{\mu - 1}{\mu_{\text{medium}}} \right) \left( \frac{1}{R_1} - \frac{1}{R_2} \right) \] where: - \( f \) is the focal length of the lens, - \( \mu \) is the refractive index of the lens, - \( \mu_{\text{medium}} \) is the refractive index of the medium in which the lens is placed, - \( R_1 \) and \( R_2 \) are the radii of curvature of the lens surfaces. ### Step 1: Focal length in air For the lens in air, the refractive index of air is approximately 1. Thus, we have: \[ \frac{1}{f} = \left( \frac{\mu - 1}{1} \right) \left( \frac{1}{R_1} - \frac{1}{R_2} \right) \] This simplifies to: \[ \frac{1}{f} = (\mu - 1) \left( \frac{1}{R_1} - \frac{1}{R_2} \right) \quad \text{(Equation 1)} \] ### Step 2: Focal length in liquid with refractive index \( \frac{\mu}{2} \) When the lens is immersed in a liquid with a refractive index of \( \frac{\mu}{2} \), we apply the lens maker's formula again: \[ \frac{1}{f_1} = \left( \frac{\mu - 1}{\frac{\mu}{2}} \right) \left( \frac{1}{R_1} - \frac{1}{R_2} \right) \] This simplifies to: \[ \frac{1}{f_1} = \left( \frac{2(\mu - 1)}{\mu} \right) \left( \frac{1}{R_1} - \frac{1}{R_2} \right) \quad \text{(Equation 2)} \] ### Step 3: Focal length in liquid with refractive index \( 2\mu \) Now, for the liquid with a refractive index of \( 2\mu \): \[ \frac{1}{f_2} = \left( \frac{\mu - 1}{2\mu} \right) \left( \frac{1}{R_1} - \frac{1}{R_2} \right) \] This simplifies to: \[ \frac{1}{f_2} = \left( \frac{\mu - 1}{2\mu} \right) \left( \frac{1}{R_1} - \frac{1}{R_2} \right) \quad \text{(Equation 3)} \] ### Step 4: Relating \( f_1 \) to \( f \) To find the relationship between \( f \) and \( f_1 \), we can divide Equation 2 by Equation 1: \[ \frac{\frac{1}{f_1}}{\frac{1}{f}} = \frac{\frac{2(\mu - 1)}{\mu} \left( \frac{1}{R_1} - \frac{1}{R_2} \right)}{(\mu - 1) \left( \frac{1}{R_1} - \frac{1}{R_2} \right)} \] This simplifies to: \[ \frac{f}{f_1} = \frac{2}{\mu} \implies f_1 = \frac{f \cdot \mu}{2} \quad \text{(Equation 4)} \] ### Step 5: Relating \( f_2 \) to \( f \) Now, we will find the relationship between \( f \) and \( f_2 \) by dividing Equation 3 by Equation 1: \[ \frac{\frac{1}{f_2}}{\frac{1}{f}} = \frac{\frac{\mu - 1}{2\mu} \left( \frac{1}{R_1} - \frac{1}{R_2} \right)}{(\mu - 1) \left( \frac{1}{R_1} - \frac{1}{R_2} \right)} \] This simplifies to: \[ \frac{f}{f_2} = \frac{1}{2\mu} \implies f_2 = 2\mu f \quad \text{(Equation 5)} \] ### Conclusion From the above relationships, we have: 1. \( f_1 = \frac{f \cdot \mu}{2} \) 2. \( f_2 = 2\mu f \) Since the values of \( \mu \) are not provided, we cannot determine the exact numerical relationships between \( f, f_1, \) and \( f_2 \). Thus, the data is insufficient to find a direct relation. ### Final Answer The correct option is **D: Data is insufficient**.
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DC PANDEY ENGLISH-RAY OPTICS-B. More than one option is correct
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  9. There are three optical media 1,2 and 3 with the refractive indices mu...

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  11. For a mirror linear magnification m comes out to +2. What conclusions ...

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  12. A convex lens made of glass (mu(g)=3//2) has focal length f in air. Th...

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  13. A converging lens is used to form an image on a screen. When the upper...

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