When the sphere is of radius \( R \), its mass is \( M \), and when the radius is reduced to \( \frac{R}{2} \), the mass will reduce to \( \frac{M}{8} \).
This is due to the conservation of angular momentum.
Using the conservation of angular momentum (\( \tau_{\text{ext}} = 0 \)): \[ I_1 \omega_1 = I_2 \omega_2 \] \[ \left( \frac{2}{5} M R^2 \right) \omega_1 = \left( \frac{2}{5} \times \frac{M}{8} \times \left( \frac{R}{2} \right)^2 \right) \omega_2 \] Simplifying this: \[ \omega_2 = 32 \omega_1 \]
Thus, the value of \( x \) is 32.
Let \( T_r \) be the \( r^{\text{th}} \) term of an A.P. If for some \( m \), \( T_m = \dfrac{1}{25} \), \( T_{25} = \dfrac{1}{20} \), and \( \displaystyle\sum_{r=1}^{25} T_r = 13 \), then \( 5m \displaystyle\sum_{r=m}^{2m} T_r \) is equal to: