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Question: \(ACB\) is a right-angled glass prism with refractive index \(1.5\). Angle \(A\), \(B\), \(C\) are \...

ACBACB is a right-angled glass prism with refractive index 1.51.5. Angle AA, BB, CC are 60{60^ \circ },30{30^ \circ }and 90{90^ \circ } respectively. A thin layer of liquid is on the ABAB. For a ray of light which is incident normally on ACAC to; be totally reflected at ABAB, the refractive index of the liquid on ABAB should be;
(A) 1.51.5
(B) 1.41.4
(C) 1.31.3
(D) 1.21.2

Explanation

Solution

The above given problem can be solved using the formula that was formulated from Snell's law of refraction with the angle of incident ray and the angle of refractive ray that comes out of the right-angled glass prism.

Formulae Used:
According to Snell’s law of refraction the refractive index of liquid is given by:
sinisinr=μμ1\dfrac{{\sin \,i}}{{\sin \,r}} = \dfrac{\mu }{{{\mu _1}}}
Where, sini\sin \,i denotes the angle of incident ray, sinr\sin \,r denotes the angle of refractive ray, μ\mu denotes the refractive index of the liquid, μ1{\mu _1} denotes the refractive index of the right-angled glass prism.

Complete step-by-step solution:

The data given in the problem is;
The refractive index of the right-angled glass prism, μ1=1.5{\mu _1} = 1.5.
From the given figure,
The angle of incidence, i=60i = {60^ \circ }.
The angle of refraction = 90{90^ \circ }.
According to Snell’s law of refraction the refractive index of liquid is:
sinisinr=μμ1\dfrac{{\sin \,i}}{{\sin \,r}} = \dfrac{\mu }{{{\mu _1}}}
Substitute the values of angle of incidence, angle of refraction, refractive index of the prism in the above equation;
31=μ1.5 μ=1.3  \dfrac{{\sqrt 3 }}{1} = \dfrac{\mu }{{1.5}} \\\ \mu = 1.3 \\\
Therefore, the refractive index of the liquid on ABAB is μ=1.3\mu = 1.3.
Hence, the option (C) μ=1.3\mu = 1.3 is the correct answer.

Note:- Snell’s law also referred to as the refractive law, is a formula used to outline the connection between the angles of incidence and angle of refraction, it represents to light passing along a boundary between two varying isotropic medium such as water, glass, or air.