Step 1: Understanding the Concept:
For a solid sphere of mass \(m\), radius \(R\), \(I = \frac25mR^2\). Using energy conservation from the top of the incline at height \(h\).
Step 2: Rolling case:
\(mgh = \frac12mV_1^2 + \frac12I\omega^2\) with \(\omega = V_1/R\):
\[ mgh = \frac12mV_1^2\left(1 + \frac25\right) = \frac12mV_1^2\cdot\frac75 \Rightarrow V_1^2 = \frac{10}{7}gh \]
Step 3: Sliding case:
No friction, so no rotation: \(mgh = \frac12mV_2^2\), giving \(V_2^2 = 2gh\).
Step 4: Ratio:
\[ \frac{V_1^2}{V_2^2} = \frac{10/7}{2} = \frac57 \Rightarrow V_1 : V_2 = \sqrt5 : \sqrt7 \]
Step 5: Why the other options are wrong.
Options (A) and (B) put the larger number first, which would make the rolling sphere faster. Rolling is slower because some energy goes into rotation. Option (C) uses \(\sqrt3\), which does not match the moment of inertia of a sphere.
Final Answer:
The ratio is \(\sqrt5 : \sqrt7\), option (D).
\[ \boxed{\sqrt{5}:\sqrt{7}} \]