| List-I | List-II | ||
| P | If \(n = 2\) and \(\alpha = 180°\), then all the possible values of \(\theta_0\) will be | I | \(30\degree\) or \(0\degree\) |
| Q | If \(n = √3\) and \(\alpha= 180°\), then all the possible values of \(\theta_0\) will be | II | \(60\degree\) or \(0\degree\) |
| R | If \(n = √3\) and \(\alpha= 180°\), then all the possible values of \(\phi_0\) will be | III | \(45\degree\) or \( 0\degree\) |
| S | If \(n = \sqrt2\) and \(\theta_0 = 45°\), then all the possible values of \(\alpha\) will be | IV | \(150\degree\) |
| \[0\degree\] | |||
Given \( n = 2 \) and \( \alpha = 180^\circ \),
\[ \delta = 2(\theta_0 - \phi_0) + \pi - 2\phi_0 = 2. \]
From the above equation, \( \phi_0 = 0^\circ \).
\[ \theta_0 = 2\phi_0 = 0^\circ. \]
Thus, \( \theta_0 = 0^\circ \) for P.
Given \( n = \sqrt{3} \) and \( \alpha = 180^\circ \),
\[ 1 \cdot \sin \theta_0 = \sqrt{3} \cdot \sin \phi_0. \]
For \( \phi_0 = 0^\circ \):
\[ \theta_0 = 0^\circ \quad \text{or} \quad \theta_0 = 60^\circ. \]
Given \( n = \sqrt{3} \) and \( \alpha = 180^\circ \), using Snell’s law:
\[ n \cdot \sin \phi_0 = \sin \theta_0. \]
Solving gives \( \phi_0 = 0^\circ \) or \( \phi_0 = 30^\circ \).
Given \( n = \sqrt{2} \) and \( \theta_0 = 45^\circ \):
\[ \sin \phi_0 = \frac{\sin 45^\circ}{\sqrt{2}} = \frac{1}{2}. \]
The total angle \( \alpha \) is:
\[ \alpha = 150^\circ. \]
Based on the calculations:
The correct option is (A).
To solve the problem, we need to analyze the refraction and reflection of light rays inside a sphere with given refractive indices and angles, then match the values from List-I with List-II.
1. Understanding the problem:
A light ray incident on the surface of a sphere partially refracts inside, reflects from the back surface, and then emerges out. Given the refractive index \(n\), angle of incidence \(\theta_0\), angle of refraction \(\phi\), and total deviation angle \(\alpha\), we find possible values of these angles under different conditions.
2. Using Snell's Law and Geometry:
Snell's Law states:
\[
n_1 \sin \theta_0 = n_2 \sin \phi
\]
For air to sphere interface, \(n_1 = 1\) and \(n_2 = n\).
Hence,
\[
\sin \theta_0 = n \sin \phi
\]
Given the total angle of deviation \(\alpha = 180^\circ\), geometrical relations help us find possible values of \(\theta_0\) and \(\phi\).
3. Matching List-I and List-II for each case:
4. Conclusion:
The correct matching is:
P → 5 (0° or 30°), Q → 2 (0° or 60°), R → 1 (0° or 45°), S → 4 (150° or 0°)
Final Answer:
Option A: P → 5; Q → 2; R → 1; S → 4
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity): 
Let $ a_0, a_1, ..., a_{23} $ be real numbers such that $$ \left(1 + \frac{2}{5}x \right)^{23} = \sum_{i=0}^{23} a_i x^i $$ for every real number $ x $. Let $ a_r $ be the largest among the numbers $ a_j $ for $ 0 \leq j \leq 23 $. Then the value of $ r $ is ________.