Since there is no external torque, angular momentum is conserved:
\[ I_1 \omega_1 = I_2 \omega_2. \]
Substitute \( I_1 = I_0 \), \( \omega_1 = \omega \), and \( I_2 = 3I_0 \):
\[ I_0 \omega = 3I_0 \omega_2. \]
Cancel \( I_0 \):
\[ \omega_2 = \frac{\omega}{3}. \]
The initial kinetic energy \( E \) is given by:
\[ E = \frac{1}{2} I_1 \omega_1^2. \]
Substitute \( I_1 = I_0 \) and \( \omega_1 = \omega \):
\[ E = \frac{1}{2} I_0 \omega^2. \]
The final kinetic energy \( E_f \) is given by:
\[ E_f = \frac{1}{2} I_2 \omega_2^2. \]
Substitute \( I_2 = 3I_0 \) and \( \omega_2 = \frac{\omega}{3} \):
\[ E_f = \frac{1}{2} (3I_0) \left(\frac{\omega}{3}\right)^2. \]
Simplify:
\[ E_f = \frac{1}{2} \cdot 3I_0 \cdot \frac{\omega^2}{9}. \]
\[ E_f = \frac{1}{6} I_0 \omega^2. \]
Compare \( E_f \) to the initial energy \( E = \frac{1}{2} I_0 \omega^2 \):
\[ E_f = \frac{1}{3} E. \]
The final kinetic energy is given as \( \frac{E}{x} \). Comparing this with \( E_f = \frac{E}{3} \), we find:
\[ x = 3. \]
The value of \( x \) is 3.
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 : \(A_2 \rightleftharpoons 2A\)