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 \( x = 2 \).
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