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Geometrical Optics question

2025 · Shift 1 · Q43
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Geometrical Optics question

2025 · Shift 1 · Q43

JEE AdvancedPhysicsGeometrical OpticsNumerical+4 / −1
A solid glass sphere of refractive index n=3n=\sqrt{3}n=3​ and radius RRR contains a spherical air cavity of radius R2\frac{R}{2}2R​, as shown in the figure. A very thin glass layer is present at the point 0 so that the air cavity (refractive index n=1n=1n=1) remains inside the glass sphere. An unpolarized, unidirectional and monochromatic light source SSS emits a light ray from a point inside the glass sphere towards the periphery of the glass sphere. If the light is reflected from the point 0 and is fully polarized, then the angle of incidence at the inner surface of the glass sphere is θ\thetaθ. The value of sin⁡θ\sin \thetasinθ is ‾\underline{\hspace{2cm}}​. JEE Advanced 2025 Paper 1 Online Physics - Geometrical Optics Question 1 English
Numerical answer
View written solutionFree

Correct answer: 0.5OR0.75

  1. Key idea: full polarization on reflection at point OOO

When light is reflected from the glass-air interface at point OOO and the reflected ray is fully polarized, the incidence at OOO must be the Brewster angle.

For light going from glass (n1=3)(n_1=\sqrt{3})(n1​=3​) to air (n2=1)(n_2=1)(n2​=1),

tan⁡iB=n2n1=13\tan i_B = \frac{n_2}{n_1} = \frac{1}{\sqrt{3}}taniB​=n1​n2​​=3​1​

Hence,

iB=30∘.i_B = 30^\circ.iB​=30∘.

So the ray inside glass strikes the cavity surface at OOO with angle of incidence 30∘30^\circ30∘.


  1. Use spherical geometry of the cavity

The air cavity has radius R2\dfrac{R}{2}2R​ and is tangent to the outer glass sphere at OOO (with a very thin glass layer there). Therefore the center of the cavity lies on the same radius through OOO.

Let:

  • CCC = center of the outer sphere,
  • C′C'C′ = center of the cavity,
  • PPP = source point,
  • OOO = point where the ray reflects from the cavity.

Since the cavity radius is R/2R/2R/2 and it is internally tangent to the outer sphere at OOO,

CC′=R−R2=R2.CC' = R - \frac{R}{2} = \frac{R}{2}.CC′=R−2R​=2R​.

Also,

C′O=R2.C'O = \frac{R}{2}.C′O=2R​.

Thus,

CO=CC′+C′O=R.CO = CC' + C'O = R.CO=CC′+C′O=R.

At point OOO, the normal to the cavity surface is along C′OC'OC′O, which is also along COCOCO. So the incident ray POPOPO makes angle 30∘30^\circ30∘ with COCOCO.


  1. Where can the source point be so that the reflected ray returns along the shown geometry?

Because the source is inside the glass sphere and the ray reflects at OOO, the relevant line from the source to OOO makes 30∘30^\circ30∘ with the radius COCOCO.

Now consider the line through OOO making angle 30∘30^\circ30∘ with COCOCO. Its perpendicular distance from the center CCC is

d=COsin⁡30∘=R⋅12=R2.d = CO \sin 30^\circ = R \cdot \frac{1}{2} = \frac{R}{2}.d=COsin30∘=R⋅21​=2R​.

That means this line is tangent to the concentric circle of radius R/2R/2R/2 centered at CCC. So the source point can correspond to the tangency point on that circle, giving

CP=R2.CP = \frac{R}{2}.CP=2R​.

Then triangle COPCOPCOP has:

  • CO=RCO=RCO=R,
  • CP=R2CP=\dfrac{R}{2}CP=2R​,
  • angle between OPOPOP and OCOCOC at OOO equal to 30∘30^\circ30∘.

This makes triangle COPCOPCOP a right triangle at PPP, and

sin⁡θ=CPCO=R/2R=12.\sin \theta = \frac{CP}{CO} = \frac{R/2}{R} = \frac{1}{2}.sinθ=COCP​=RR/2​=21​.

So,

sin⁡θ=12.\boxed{\sin\theta = \frac{1}{2}}.sinθ=21​​.
  1. Comparison with stored answer

Stored correct answer: 0.5 OR 0.75

Our derived answer is

sin⁡θ=12=0.5.\sin\theta = \frac{1}{2} = 0.5.sinθ=21​=0.5.

So it matches one of the accepted stored answers.

Next

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