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Geometrical Optics question

2024 · Shift 2 · Q45
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Geometrical Optics question

2024 · Shift 2 · Q45

JEE AdvancedPhysicsGeometrical OpticsNumerical+4 / −1
Two equilateral-triangular prisms P1\mathrm{P}_1P1​ and P2\mathrm{P}_2P2​ are kept with their sides parallel to each other, in vacuum, as shown in the figure. A light ray enters prism P1\mathrm{P}_1P1​ at an angle of incidence θ\thetaθ such that the outgoing ray undergoes minimum deviation in prism P2\mathrm{P}_2P2​. If the respective refractive indices of P1\mathrm{P}_1P1​ and P2\mathrm{P}_2P2​ are 32\sqrt{\frac{3}{2}}23​​ and 3\sqrt{3}3​, then θ=sin⁡−1[32sin⁡(πβ)]\theta=\sin ^{-1}\left[\sqrt{\frac{3}{2}} \sin \left(\frac{\pi}{\beta}\right)\right]θ=sin−1[23​​sin(βπ​)], where the value of β\betaβ is ‾\underline{\hspace{2cm}}​. JEE Advanced 2024 Paper 2 Online Physics - Geometrical Optics Question 5 English
Numerical answer
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Correct answer: 12

  1. Given data
  • Both prisms are equilateral, so prism angle A=60∘.A=60^\circ.A=60∘.
  • Refractive indices: μ1=32,μ2=3.\mu_1=\sqrt{\frac32},\qquad \mu_2=\sqrt3.μ1​=23​​,μ2​=3​.
  • The ray emerging from prism P1P_1P1​ enters prism P2P_2P2​.
  • It is given that in prism P2P_2P2​, the ray undergoes minimum deviation.

  1. Condition for minimum deviation in P2P_2P2​

For a prism at minimum deviation, r1=r2=A2=30∘.r_1=r_2=\frac{A}{2}=30^\circ.r1​=r2​=2A​=30∘.

So, inside prism P2P_2P2​, the angle of refraction at the first face must be 30∘30^\circ30∘.

Applying Snell's law at the first face of P2P_2P2​ (vacuum to prism): sin⁡i2=μ2sin⁡30∘\sin i_2=\mu_2\sin 30^\circsini2​=μ2​sin30∘ where i2i_2i2​ is the angle of incidence on prism P2P_2P2​ from vacuum.

Thus, sin⁡i2=3⋅12=32\sin i_2=\sqrt3\cdot \frac12=\frac{\sqrt3}{2}sini2​=3​⋅21​=23​​ so i2=60∘.i_2=60^\circ.i2​=60∘.

Hence, the ray must strike the first face of P2P_2P2​ at angle 60∘60^\circ60∘ to the normal.


  1. Relating this to the ray emerging from P1P_1P1​

Since the corresponding faces of the two prisms are parallel, the normal to the second face of P1P_1P1​ is parallel to the normal to the first face of P2P_2P2​.

Therefore, the angle of emergence from P1P_1P1​ into vacuum must be e1=i2=60∘.e_1=i_2=60^\circ.e1​=i2​=60∘.


  1. Refraction at the second face of P1P_1P1​

Let the internal angle of incidence at the second face of P1P_1P1​ be r2r_2r2​.

Using Snell's law from prism P1P_1P1​ to vacuum: μ1sin⁡r2=sin⁡e1\mu_1\sin r_2=\sin e_1μ1​sinr2​=sine1​ 32sin⁡r2=sin⁡60∘=32.\sqrt{\frac32}\sin r_2=\sin 60^\circ=\frac{\sqrt3}{2}.23​​sinr2​=sin60∘=23​​.

So, sin⁡r2=3/23/2=12.\sin r_2=\frac{\sqrt3/2}{\sqrt{3/2}}=\frac{1}{\sqrt2}.sinr2​=3/2​3​/2​=2​1​. Hence, r2=45∘.r_2=45^\circ.r2​=45∘.


  1. Use prism relation for P1P_1P1​

For prism P1P_1P1​, r1+r2=A=60∘.r_1+r_2=A=60^\circ.r1​+r2​=A=60∘. Thus, r1=60∘−45∘=15∘.r_1=60^\circ-45^\circ=15^\circ.r1​=60∘−45∘=15∘.


  1. Refraction at the first face of P1P_1P1​

Let the external angle of incidence be θ\thetaθ.

By Snell's law (vacuum to prism P1P_1P1​): sin⁡θ=μ1sin⁡r1\sin\theta=\mu_1\sin r_1sinθ=μ1​sinr1​ sin⁡θ=32sin⁡15∘.\sin\theta=\sqrt{\frac32}\sin 15^\circ.sinθ=23​​sin15∘.

So, θ=sin⁡−1[32sin⁡15∘].\theta=\sin^{-1}\left[\sqrt{\frac32}\sin 15^\circ\right].θ=sin−1[23​​sin15∘].

This is of the form θ=sin⁡−1[32sin⁡(πβ)].\theta=\sin^{-1}\left[\sqrt{\frac32}\sin\left(\frac{\pi}{\beta}\right)\right].θ=sin−1[23​​sin(βπ​)].

Therefore, πβ=15∘=π12\frac{\pi}{\beta}=15^\circ=\frac{\pi}{12}βπ​=15∘=12π​ which gives β=12.\beta=12.β=12.


  1. Final answer

12\boxed{12}12​

The derived answer matches the stored correct answer.

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