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Geometrical Optics question

2020 · 3 Sep · Shift 1 · Q43
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Geometrical Optics question

2020 · 3 Sep · Shift 1 · Q43

JEE MainPhysicsGeometrical OpticsNumerical+4 / −1
An observer can see through a small hole on the side of a jar (radius 15 cm) at a point at height of 15 cm from the bottom (see figure). The hole is at a height of 45 cm. When the jar is filled with a liquid up to a height of 30 cm the same observer can see the edge at the bottom of the jar. If the refractive index of the liquid is N/100, where N is an integer, the value of N is ‾\underline{\hspace{2cm}}​. JEE Main 2020 (Online) 3rd September Morning Slot Physics - Geometrical Optics Question 165 English
Numerical answer
View written solutionFree

Correct answer: 158

  1. Interpret the geometry

    The jar has radius 15 cm15\text{ cm}15 cm, so its diameter is 30 cm.30\text{ cm}.30 cm.

    The observer looks through a small hole on the side wall at height 45 cm45\text{ cm}45 cm from the bottom.

    The liquid is filled up to height 30 cm30\text{ cm}30 cm.

    After filling, the observer can see the edge at the bottom of the jar on the opposite side. So the light ray travels:

    • from the bottom edge on one side,
    • through the liquid up to the liquid surface,
    • then through air to the hole.
  2. Path of the ray in air

    The refracted ray emerges from the liquid surface and reaches the hole.

    The hole is at height 45 cm45\text{ cm}45 cm, while the liquid surface is at height 30 cm30\text{ cm}30 cm, so vertical rise in air is 45−30=15 cm.45-30 = 15\text{ cm}.45−30=15 cm.

    The horizontal distance from the point where the ray emerges at the surface to the hole-side wall is 15 cm15\text{ cm}15 cm if the emergence point is vertically above the center of the jar. This is the limiting ray that allows the opposite bottom edge to be seen.

    Thus, in air, tan⁡r=1515=1  ⟹  r=45∘.\tan r = \frac{15}{15}=1 \implies r=45^\circ.tanr=1515​=1⟹r=45∘.

    Here rrr is the angle of refraction with the normal (normal is vertical).

  3. Path of the ray in liquid

    The bottom edge seen is the opposite edge, so inside the liquid the ray goes from that bottom edge to the point on the surface directly above the center.

    Hence, horizontal displacement in liquid is 15 cm15\text{ cm}15 cm and vertical rise is 30 cm30\text{ cm}30 cm.

    Therefore, tan⁡i=1530=12,\tan i = \frac{15}{30}=\frac12,tani=3015​=21​, where iii is the angle of incidence in liquid with the vertical normal.

    So, sin⁡i=15.\sin i = \frac{1}{\sqrt{5}}.sini=5​1​.

  4. Apply Snell's law

    For refraction from liquid to air, μsin⁡i=sin⁡r,\mu \sin i = \sin r,μsini=sinr, where μ\muμ is the refractive index of the liquid.

    Substituting: μ⋅15=sin⁡45∘=12.\mu \cdot \frac{1}{\sqrt{5}} = \sin 45^\circ = \frac{1}{\sqrt{2}}.μ⋅5​1​=sin45∘=2​1​.

    Hence, μ=52=52.\mu = \frac{\sqrt{5}}{\sqrt{2}} = \sqrt{\frac52}.μ=2​5​​=25​​.

    Numerically, μ≈1.581.\mu \approx 1.581.μ≈1.581.

  5. Find NNN

    Given refractive index is N100\dfrac{N}{100}100N​, N100≈1.581  ⟹  N≈158.1.\frac{N}{100} \approx 1.581 \implies N \approx 158.1.100N​≈1.581⟹N≈158.1.

    Since NNN is an integer, N=158.N=158.N=158.

  6. Comparison with stored answer

    Stored correct answer = 158158158.

    This matches our derived answer.

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