For rolling motion, always use the rolling condition \( v = R \omega \) to simplify relationships between energy, angular momentum, and angular speed.
For a solid sphere rolling without slipping:
The total energy is the sum of translational kinetic energy and rotational kinetic energy: \[ E_{\text{total}} = \frac{1}{2} M v^2 + \frac{1}{2} I \omega^2 \] where \( I = \frac{2}{5} M R^2 \) is the moment of inertia of the sphere about its axis of rotation.
Using the rolling condition \( v = R \omega \), the total energy becomes: \[ E_{\text{total}} = \frac{1}{2} M v^2 + \frac{1}{2} \left( \frac{2}{5} M R^2 \right) \omega^2 = \frac{7}{10} M v^2 \]
The angular momentum about the axis of rotation is: \[ L = I \omega = \frac{2}{5} M R^2 \omega. \] Given that the ratio of angular momentum to total energy is \( \pi : 22 \): \[ \frac{L}{E_{\text{total}}} = \frac{\pi}{22} \] Substitute the expressions for \( L \) and \( E_{\text{total}} \): \[ \frac{\frac{2}{5} M R^2 \omega}{\frac{7}{10} M v^2} = \frac{\pi}{22} \] Simplify using \( v = R \omega \): \[ \frac{\frac{2}{5} M R^2 \omega}{\frac{7}{10} M (R \omega)^2} = \frac{\pi}{22} \] Cancel terms: \[ \frac{\frac{2}{5}}{\frac{7}{10} R \omega} = \frac{\pi}{22} \] Solve for \( \omega \): \[ \omega = \frac{22 \times \frac{2}{5}}{\pi \times \frac{7}{10} R} \] Simplify: \[ \omega = \frac{4}{\pi R} \quad \text{rad/s} \]
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,

What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)