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The diagram below shows a fish in the tank and its image seen in the surface of water.

The diagram shows a fish in the tank and its image seen in the surface of water. Name the phenomenon responsible for the formation of this image. ICSE 2025 Specimen Physics Solved Question Paper.

(a) Name the phenomenon responsible for the formation of this image.

(b) A double convex lens with refractive index μ1 inside two liquids of refractive indices μ2 and μ3 are shown in the diagrams below. The refractive indices are such that μ2 > μ1 and μ1 > μ3

A double convex lens with refractive index μ1 inside two liquids of refractive indices μ2 and μ3 are shown in the diagrams below. ICSE 2025 Specimen Physics Solved Question Paper.

How would a parallel incident beam of light refract when it comes out of the lens in each of the cases shown above?

(1) in figure a.

(2) in figure b.

Refraction Plane Surfaces

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Answer

(a) Total internal reflection.

(b) According to the lens maker formula :

1f(refractive index of 2nd mediumrefractive index of 1st medium1)\dfrac{1}{\text f} ∝ \left(\dfrac {\text {refractive index of 2nd medium}}{\text {refractive index of 1st medium} } - 1\right) ……(i)

(1) In figure a :

Refractive index of 1st medium = μ3

Refractive index of 2nd medium = μ1

Then ,from relation (i)

1f(μ1μ31)\dfrac{1}{\text f} ∝ \left(\dfrac {\text μ1 }{\text μ3} - 1\right)

As,

μ1 > μ3

μ1μ3>11f>0f>0\Rightarrow \dfrac{\text μ1}{\text μ3} \gt 1 \\[1 em] \Rightarrow \dfrac{1}{\text f} \gt 0 \\[1 em] \Rightarrow \text f \gt 0

Since, the resulting focal length is positive so this lens behaves as a converging lens.

Hence, a parallel incident beam of light converges when it comes out of the lens im figure a.

(2) In figure b :

Refractive index of 1st medium = μ2

Refractive index of 2nd medium = μ1

Then, from relation (i)

1f(μ1μ21)\dfrac{1}{\text f} ∝ \left(\dfrac {\text μ1 }{\text μ2} - 1\right)

As,

μ1 < μ2

μ1μ2<11f<0f<0\Rightarrow \dfrac{\text μ1}{\text μ2} \lt 1 \\[1 em] \Rightarrow \dfrac{1}{\text f} \lt 0 \\[1 em] \Rightarrow \text f \lt 0

Since, the resulting focal length is negative so this lens behaves as a diverging lens.

Hence, a parallel incident beam of light diverges when it comes out of the lens im figure b.

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