For a solid sphere undergoing pure rolling motion, its total kinetic energy \( K_{\text{total}} \) is the sum of its translational kinetic energy and rotational kinetic energy.
- The translational kinetic energy of the center of mass is given by:
\[
K_{\text{linear}} = \frac{1}{2} m v^2,
\]
where \( m \) denotes the mass of the sphere and \( v \) represents the linear velocity of the center of mass.
- The rotational kinetic energy is expressed as:
\[
K_{\text{rotational}} = \frac{1}{2} I \omega^2,
\]
where \( I \) is the moment of inertia and \( \omega \) is the angular velocity. For a solid sphere, the moment of inertia about its center of mass is:
\[
I = \frac{2}{5} m r^2,
\]
where \( r \) signifies the radius of the sphere.
Given that the sphere is rolling without slipping, the relationship between linear and angular velocity is \( v = r \omega \). Consequently, the rotational kinetic energy can be rewritten as:
\[
K_{\text{rotational}} = \frac{1}{2} \times \frac{2}{5} m r^2 \times \left( \frac{v}{r} \right)^2 = \frac{1}{5} m v^2.
\]
The ratio of the translational kinetic energy to the rotational kinetic energy is calculated as follows:
\[
\text{Ratio} = \frac{K_{\text{linear}}}{K_{\text{rotational}}} = \frac{\frac{1}{2} m v^2}{\frac{1}{5} m v^2} = \frac{5}{2}.
\]
Final Answer: The ratio is \( \frac{5}{2} \).