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Geometrical Optics question

2025 · 7 Apr · Shift 2 · Q68
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Geometrical Optics question

2025 · 7 Apr · Shift 2 · Q68

JEE MainPhysicsGeometrical OpticsMCQ+4 / −1
A transparent block A having refractive index μ=1.25\mu = 1.25μ=1.25 is surrounded by another medium of refractive index μ=1.0\mu = 1.0μ=1.0 as shown in the figure. A light ray is incident on the flat face of the block with incident angle θ\thetaθ as shown in the figure. What is the maximum value of θ\thetaθ for which light suffers total internal reflection at the top surface of the block? JEE Main 2025 (Online) 7th April Evening Shift Physics - Geometrical Optics Question 7 English
  1. A
    tan⁡−1(4/3)\tan^{-1}(4/3)tan−1(4/3)
  2. B
    sin⁡−1(3/4)\sin^{-1}(3/4)sin−1(3/4)
  3. C
    tan⁡−1(3/4)\tan^{-1}(3/4)tan−1(3/4)
  4. D
    cos⁡−1(3/4)\cos^{-1}(3/4)cos−1(3/4)
View written solutionFree

Correct answer: B

  1. Given data
  • Refractive index of block: μ1=1.25=54\mu_1 = 1.25 = \dfrac{5}{4}μ1​=1.25=45​
  • Refractive index of surrounding medium: μ2=1\mu_2 = 1μ2​=1
  • A ray enters through the vertical flat face and then strikes the top horizontal surface.

We need the maximum incident angle θ\thetaθ at the side face such that the ray undergoes total internal reflection (TIR) at the top surface.


  1. Refraction at the side face

Let the angle of refraction inside the block at the side face be rrr.

Since the ray is entering from medium (μ=1)(\mu=1)(μ=1) into the block (μ=1.25)(\mu=1.25)(μ=1.25), Snell's law gives:

1⋅sin⁡θ=1.25 sin⁡r1\cdot \sin\theta = 1.25\,\sin r1⋅sinθ=1.25sinr sin⁡θ=54sin⁡r\sin\theta = \frac{5}{4}\sin rsinθ=45​sinr
  1. Condition for total internal reflection at the top surface

At the top surface, the ray goes from denser medium (1.25)(1.25)(1.25) to rarer medium (1)(1)(1).

Critical angle ccc satisfies:

sin⁡c=μ2μ1=11.25=45\sin c = \frac{\mu_2}{\mu_1} = \frac{1}{1.25} = \frac{4}{5}sinc=μ1​μ2​​=1.251​=54​

So,

c=sin⁡−1(45)c = \sin^{-1}\left(\frac{4}{5}\right)c=sin−1(54​)

Now, if the ray makes angle rrr with the horizontal normal of the side face, then at the top horizontal surface its angle of incidence is:

i=90∘−ri = 90^\circ - ri=90∘−r

For just TIR (maximum θ\thetaθ),

i=ci = ci=c

Hence,

90∘−r=c90^\circ - r = c90∘−r=c r=90∘−cr = 90^\circ - cr=90∘−c

Using

sin⁡c=45  ⟹  cos⁡c=35\sin c = \frac{4}{5} \implies \cos c = \frac{3}{5}sinc=54​⟹cosc=53​

therefore,

sin⁡r=sin⁡(90∘−c)=cos⁡c=35\sin r = \sin(90^\circ - c) = \cos c = \frac{3}{5}sinr=sin(90∘−c)=cosc=53​
  1. Find maximum θ\thetaθ

From Snell's law:

sin⁡θ=54sin⁡r=54⋅35=34\sin\theta = \frac{5}{4}\sin r = \frac{5}{4}\cdot \frac{3}{5} = \frac{3}{4}sinθ=45​sinr=45​⋅53​=43​

Thus,

θmax⁡=sin⁡−1(34)\theta_{\max} = \sin^{-1}\left(\frac{3}{4}\right)θmax​=sin−1(43​)
  1. Check options
  • A: tan⁡−1(4/3)\tan^{-1}(4/3)tan−1(4/3) — incorrect
  • B: sin⁡−1(3/4)\sin^{-1}(3/4)sin−1(3/4) — correct
  • C: tan⁡−1(3/4)\tan^{-1}(3/4)tan−1(3/4) — incorrect
  • D: cos⁡−1(3/4)\cos^{-1}(3/4)cos−1(3/4) — incorrect

So the correct option is B.

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