Step 1:
When an object rolls without slipping, its total kinetic energy is the sum of its translational kinetic energy and its rotational kinetic energy. The total kinetic energy is:
\[
K_{\text{total}} = K_{\text{trans}} + K_{\text{rot}}
\]
Step 2:
For a solid cylinder rolling without slipping, the rotational kinetic energy is related to the translational kinetic energy by:
\[
K_{\text{rot}} = \frac{1}{2} I \omega^2
\]
where \( I = \frac{1}{2} m r^2 \) is the moment of inertia for a solid cylinder and \( \omega = \frac{v}{r} \) is the angular velocity. Thus,
\[
K_{\text{rot}} = \frac{1}{2} m v^2
\]
Therefore, the total kinetic energy becomes:
\[
K_{\text{total}} = K_{\text{trans}} + \frac{1}{2} K_{\text{trans}} = \frac{3}{2} K_{\text{trans}}
\]
Step 3:
Given that \( K_{\text{trans}} = 140 \, \text{J} \), the total kinetic energy is:
\[
K_{\text{total}} = \frac{3}{2} \times 140 = 210 \, \text{J}
\]
Thus, the total kinetic energy of the cylinder is 210 J.