Step 1: Use the ratio of translational to rotational energy:
For rolling bodies $\frac{K_T}{K_R} = \frac{mR^2}{I}$. For a solid sphere $I = \frac25mR^2$, so $\frac{K_T}{K_R} = \frac52$.
Step 2: Add one:
$\frac{K_{total}}{K_R} = \frac{K_T + K_R}{K_R} = \frac52 + 1 = \frac72$.
Step 3: Remark:
The inclined plane angle does not matter. The ratio comes only from the shape of the body, since $v = \omega R$ ties translation to rotation.
Final Answer:
$\frac72$, option (B).
\[ \boxed{\frac{7}{2} \text{ (B)}} \]