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Question: A ray of light is incident from a denser to a rarer medium. The critical angle for total internal re...

A ray of light is incident from a denser to a rarer medium. The critical angle for total internal reflection is θiC{\theta _{iC}} ​ and the Brewster's angle of incidence is θiB{\theta _{iB}} ​, such that sinθiC/sinθiB=n=1.28sin{\theta _{iC}}/sin{\theta _{iB}} = n = 1.28. The relative refractive index of the two media is:
A) 0.20.2
B) 0.40.4
C) 0.80.8
D) 0.90.9

Explanation

Solution

Hint The critical angle for total internal reflection and the Brewster angle of incidence are both related to the ratio of the refractive index of the denser to the rarer medium. Find the Brewster angle in terms of sinθiB\sin {\theta _{iB}} and take its ratio with the critical angle.

Formula used:
-Critical angle of incidence: sinθiC=n2n1\sin {\theta _{iC}} = \dfrac{{{n_2}}}{{{n_1}}}
- Brewster’s angle of incidence: tanθiC=n2n1\tan {\theta _{iC}} = \dfrac{{{n_2}}}{{{n_1}}}

Complete step by step answer
The critical angle of incidence θic{\theta _{ic}} is the highest incident angle possible after which the light ray will be deflected by the denser medium than getting refracted.
So we have
sinθiC=n2n1\Rightarrow \sin {\theta _{iC}} = \dfrac{{{n_2}}}{{{n_1}}}
If a ray of light is incident at an interface between two media in such a manner that the reflected and transmitted rays are at right angles to each other, the angle of incidence is called the Brewster angle and it is defined as:
tanθiC=n2n1\Rightarrow \tan {\theta _{iC}} = \dfrac{{{n_2}}}{{{n_1}}}
We can calculate sinθiB\sin {\theta _{iB}} from tanθiB\tan {\theta _{iB}} as
sinθiB=n2(n12+n22)\Rightarrow sin{\theta _{iB}} = \dfrac{{{n_2}}}{{\sqrt {\left( {n_1^2 + n_2^2} \right)} }}
But since we want to find the ratio of
sinθiC/sinθiB\Rightarrow sin{\theta _{iC}}/sin{\theta _{iB}} , we can write
sinθiC/sinθiB=n2n1n2(n12+n22)=1.28\Rightarrow sin{\theta _{iC}}/sin{\theta _{iB}} = \dfrac{{\dfrac{{{n_2}}}{{{n_1}}}}}{{\dfrac{{{n_2}}}{{\sqrt {\left( {n_1^2 + n_2^2} \right)} }}}} = 1.28
Taking the square on both sides, we get
n22n12n22n12+n22=1.6384\Rightarrow \dfrac{{\dfrac{{n_2^2}}{{n_1^2}}}}{{\dfrac{{n_2^2}}{{n_1^2 + n_2^2}}}} = 1.6384
On simplifying, we get
n12+n22n12=1.6384\Rightarrow \dfrac{{n_1^2 + n_2^2}}{{n_1^2}} = 1.6384
Multiplying both sides n12n_1^2 and taking the terms containing n12n_1^2 on one side, we get
n22n12=0.6384\Rightarrow \dfrac{{n_2^2}}{{n_1^2}} = 0.6384
Taking the square root on both sides, we get
n2n1=0.8\dfrac{{{n_2}}}{{{n_1}}} = 0.8 which corresponds to option (C).

Note
To solve such questions, we must be aware of the different phenomena about refraction of light in different mediums such as total internal reflection and Brewster’s angle of incidence. Also, since we’ve been asked about the relative refractive index, we only have to find the ratio of the refractive index of the two mediums and not individually.