Solution:
For a rolling spherical shell, the angular velocity \( \omega = \frac{v}{R} \).
The rotational kinetic energy is given by:
\[
K_{\text{rot}} = \frac{1}{2} \left( \frac{2}{3} m R^2 \right) \left( \frac{v}{R} \right)^2 = \frac{1}{2} \left( \frac{2}{3} m R^2 \right) \left( \frac{v^2}{R^2} \right) = \frac{1}{3} m v^2.
\]
The total kinetic energy is:
\[
K_{\text{total}} = \frac{1}{2} mv^2 + \frac{1}{2} \left( \frac{2}{3} m R^2 \right) \left( \frac{v}{R} \right)^2 = \frac{1}{2} mv^2 + \frac{1}{3} mv^2 = \frac{5}{6} mv^2.
\]
The ratio of rotational kinetic energy to total kinetic energy is:
\[
\frac{K_{\text{rot}}}{K_{\text{total}}} = \frac{\frac{1}{3} m v^2}{\frac{5}{6} m v^2} = \frac{2}{5}.
\]
Thus, \( \frac{x}{5} = \frac{2}{5} \), so \( x = 2 \).
A bob of mass \(m\) is suspended at a point \(O\) by a light string of length \(l\) and left to perform vertical motion (circular) as shown in the figure. Initially, by applying horizontal velocity \(v_0\) at the point ‘A’, the string becomes slack when the bob reaches at the point ‘D’. The ratio of the kinetic energy of the bob at the points B and C is: 

Let \( a \in \mathbb{R} \) and \( A \) be a matrix of order \( 3 \times 3 \) such that \( \det(A) = -4 \) and \[ A + I = \begin{bmatrix} 1 & a & 1 \\ 2 & 1 & 0 \\ a & 1 & 2 \end{bmatrix} \] where \( I \) is the identity matrix of order \( 3 \times 3 \).
If \( \det\left( (a + 1) \cdot \text{adj}\left( (a - 1) A \right) \right) \) is \( 2^m 3^n \), \( m, n \in \{ 0, 1, 2, \dots, 20 \} \), then \( m + n \) is equal to: