Question:

At the interface between two materials having refractive indices \( n_1 \) and \( n_2 \), the critical angle for reflection of an EM wave is \( \theta_c \). The \( n_1 \) material is replaced by another material having refractive index \( n_3 \), such that the critical angle at the interface between \( n_1 \) and \( n_3 \) materials is \( \theta_{c3} \). If \( n_1 > n_2 > n_3 \), \( \frac{n_2}{n_3} = \frac{2}{5} \), and \( \sin \theta_{c2} - \sin \theta_{c1} = \frac{1}{2} \), then \( \theta_{c1} \) is:

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For problems involving critical angles and refractive indices, use Snell's Law and the relationship between the angles to find the unknowns.
Updated On: Mar 24, 2025
  • \( \sin^{-1} \left( \frac{5}{6n_1} \right) \)
  • \( \sin^{-1} \left( \frac{2}{3n_1} \right) \)
  • \( \sin^{-1} \left( \frac{1}{3n_1} \right) \)
  • \( \sin^{-1} \left( \frac{1}{6n_1} \right) \)
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The Correct Option is A

Solution and Explanation

Using the given relations for the critical angle and refractive indices, we can derive the expression for \( \theta_{c1} \). The critical angle is related to the refractive index by the equation \( \sin \theta_c = \frac{n_2}{n_1} \), and the difference between the sines of the critical angles for the two interfaces gives the desired result.
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