| 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 reaction sequence given below is carried out with 16 moles of X. The yield of the major product in each step is given below the product in parentheses. The amount (in grams) of S produced is ____. 
Use: Atomic mass (in amu): H = 1, C = 12, O = 16, Br = 80
Let $ \mathbb{R} $ denote the set of all real numbers. Then the area of the region $$ \left\{ (x, y) \in \mathbb{R} \times \mathbb{R} : x > 0, y > \frac{1}{x},\ 5x - 4y - 1 > 0,\ 4x + 4y - 17 < 0 \right\} $$ is
As shown in the figures, a uniform rod $ OO' $ of length $ l $ is hinged at the point $ O $ and held in place vertically between two walls using two massless springs of the same spring constant. The springs are connected at the midpoint and at the top-end $ (O') $ of the rod, as shown in Fig. 1, and the rod is made to oscillate by a small angular displacement. The frequency of oscillation of the rod is $ f_1 $. On the other hand, if both the springs are connected at the midpoint of the rod, as shown in Fig. 2, and the rod is made to oscillate by a small angular displacement, then the frequency of oscillation is $ f_2 $. Ignoring gravity and assuming motion only in the plane of the diagram, the value of $\frac{f_1}{f_2}$ is: