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 wheel of radius $ 0.2 \, \text{m} $ rotates freely about its center when a string that is wrapped over its rim is pulled by a force of $ 10 \, \text{N} $. The established torque produces an angular acceleration of $ 2 \, \text{rad/s}^2 $. Moment of inertia of the wheel is............. kg m².

In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by: