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Geometrical Optics question

2017 · 8 Apr · Shift 1 · Q51
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Geometrical Optics question

2017 · 8 Apr · Shift 1 · Q51

JEE MainPhysicsGeometrical OpticsMCQ+4 / −1
Let the refractive index of a denser medium with respect to a rarer medium be n12 and its critical angle be θC . At an angle of incidence A when light is travelling from denser medium to rarer medium, a part of the light is reflected and the rest is refracted and the angle between reflected and refracted rays is 90o. Angle A is given by :
  1. A
    1cos⁡−1(sin⁡θC){1 \over {{{\cos }^{ - 1}}\left( {\sin {\theta _C}} \right)}}cos−1(sinθC​)1​
  2. B
    1tan⁡−1(sin⁡θC){1 \over {{{\tan }^{ - 1}}\left( {\sin {\theta _C}} \right)}}tan−1(sinθC​)1​
  3. C
    cos⁡−1 (sin⁡θC){\cos ^{ - 1}}\,\left( {\sin {\theta _C}} \right)cos−1(sinθC​)
  4. D
    tan⁡−1 (sin⁡θC){\tan ^{ - 1}}\,\left( {\sin {\theta _C}} \right)tan−1(sinθC​)
View written solutionFree

Correct answer: D

  1. Given condition: reflected and refracted rays are perpendicular
    When the angle between the reflected ray and refracted ray is 90∘90^\circ90∘, the incidence angle is the Brewster angle for the given pair of media.

So, i+r=90∘i+r=90^\circi+r=90∘ where i=Ai=Ai=A and rrr is the angle of refraction.

  1. Apply Snell’s law
    Light goes from denser medium to rarer medium. If refractive index of denser medium with respect to rarer medium is n12n_{12}n12​, then n12=sin⁡rsin⁡in_{12}=\frac{\sin r}{\sin i}n12​=sinisinr​

Using r=90∘−ir=90^\circ-ir=90∘−i, n12=sin⁡(90∘−i)sin⁡i=cos⁡isin⁡i=cot⁡in_{12}=\frac{\sin(90^\circ-i)}{\sin i}=\frac{\cos i}{\sin i}=\cot in12​=sinisin(90∘−i)​=sinicosi​=coti

Hence, tan⁡i=1n12\tan i=\frac{1}{n_{12}}tani=n12​1​

So, A=i=tan⁡−1(1n12)A=i=\tan^{-1}\left(\frac{1}{n_{12}}\right)A=i=tan−1(n12​1​)

  1. Use the critical angle relation
    For critical angle θC\theta_CθC​ when light goes from denser to rarer medium, sin⁡θC=1n12\sin\theta_C=\frac{1}{n_{12}}sinθC​=n12​1​

Substitute into the above expression: A=tan⁡−1(sin⁡θC)A=\tan^{-1}(\sin\theta_C)A=tan−1(sinθC​)

  1. Match with the options
    This is exactly Option D.

Therefore, A=tan⁡−1(sin⁡θC)\boxed{A=\tan^{-1}(\sin\theta_C)}A=tan−1(sinθC​)​

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