For a solid sphere rolling without slipping, the total kinetic energy is the sum of translational and rotational kinetic energies.
1. The translational kinetic energy \( K_{\text{trans}} \) is given by:
\[
K_{\text{trans}} = \frac{1}{2} m v^2
\]
where \( m \) is the mass and \( v \) is the velocity of the center of mass.
2. The rotational kinetic energy \( K_{\text{rot}} \) is given by:
\[
K_{\text{rot}} = \frac{1}{2} I \omega^2
\]
where \( I \) is the moment of inertia of the sphere and \( \omega \) is the angular velocity.
For a solid sphere, the moment of inertia about the center is:
\[
I = \frac{2}{5} m r^2
\]
where \( r \) is the radius of the sphere.
Since the sphere rolls without slipping, the relation between the linear velocity and angular velocity is:
\[
v = r \omega
\]
Substituting \( \omega = \frac{v}{r} \) into the rotational kinetic energy formula:
\[
K_{\text{rot}} = \frac{1}{2} \times \frac{2}{5} m r^2 \times \left(\frac{v}{r}\right)^2 = \frac{1}{5} m v^2
\]
Now, the ratio of translational kinetic energy to rotational kinetic energy is:
\[
\frac{K_{\text{trans}}}{K_{\text{rot}}} = \frac{\frac{1}{2} m v^2}{\frac{1}{5} m v^2} = \frac{5}{2} \times \frac{1}{2} = \frac{5}{4}
\]
Thus, the ratio of translational to rotational kinetic energy is \( \frac{3}{4} \).