
Using the Work-Energy Theorem (W.E.T.) from point A to point B:
1. Apply W.E.T. from A to B:
\[ W_{mg} = K_B - K_A. \] Since the body starts from rest at A, \( K_A = 0 \). Thus,
\[ mg \times \left( \frac{R}{\sqrt{2}} + R \right) = \frac{1}{2} mv_B^2. \]
2. Substitute Values and Solve for \( v_B \):
Simplifying, we get:
\[ mgR \frac{(\sqrt{2} + 1)}{\sqrt{2}} = \frac{1}{2} mv_B^2. \] Solving for \( v_B \), we find:
\[ v_B = \sqrt{\frac{2gR(\sqrt{2} + 1)}{\sqrt{2}}}. \] Substitute \( g = 10 \, \text{m/s}^2 \), \( R = 14 \, \text{m} \), and \( \sqrt{2} = 1.4 \):
\[ v_B = \sqrt{\frac{2 \times 10 \times 14 \times 2.4}{1.4}} = 21.9 \, \text{m/s}. \]
Answer: 21.9 m/s
Consider the following sequence of reactions : 
Molar mass of the product formed (A) is ______ g mol\(^{-1}\).
In a Young's double slit experiment, three polarizers are kept as shown in the figure. The transmission axes of \( P_1 \) and \( P_2 \) are orthogonal to each other. The polarizer \( P_3 \) covers both the slits with its transmission axis at \( 45^\circ \) to those of \( P_1 \) and \( P_2 \). An unpolarized light of wavelength \( \lambda \) and intensity \( I_0 \) is incident on \( P_1 \) and \( P_2 \). The intensity at a point after \( P_3 \), where the path difference between the light waves from \( S_1 \) and \( S_2 \) is \( \frac{\lambda}{3} \), is:
