For a solid sphere rolling without slipping, the total kinetic energy is the sum of translational kinetic energy and rotational kinetic energy. The total kinetic energy \( K \) is given by:
\[
K = \frac{1}{2} mv^2 + \frac{1}{2} I \omega^2
\]
where \( m \) is the mass, \( v \) is the velocity, \( I \) is the moment of inertia of the sphere, and \( \omega \) is the angular velocity.
For a solid sphere, the moment of inertia \( I = \frac{2}{5} m r^2 \), and the relationship between linear and angular velocity for rolling without slipping is \( v = r \omega \).
Thus, the rotational kinetic energy is \( \frac{1}{2} I \omega^2 = \frac{1}{2} \times \frac{2}{5} m r^2 \times \left( \frac{v}{r} \right)^2 = \frac{1}{5} m v^2 \).
The total kinetic energy is:
\[
K = \frac{1}{2} m v^2 + \frac{1}{5} m v^2 = \frac{7}{10} m v^2
\]
The translational kinetic energy is \( \frac{1}{2} m v^2 \).
Therefore, the ratio of translational to rotational kinetic energy is:
\[
\frac{\frac{1}{2} m v^2}{\frac{1}{5} m v^2} = \frac{5}{2}
\]
Thus, the ratio of translational to rotational kinetic energy is \( 5:2 \).