Step 1: Energy considerations.
The solid cylinder rolls down the inclined plane, so its total mechanical energy is conserved. Initially, the cylinder has potential energy \( mgh \), and at the bottom, this energy is converted into kinetic energy, which consists of both translational and rotational kinetic energy. The total kinetic energy is given by:
\[
K.E. = \frac{1}{2} M v^2 + \frac{1}{2} I \omega^2
\]
For a solid cylinder, the moment of inertia \( I \) is \( \frac{1}{2} M R^2 \), and the angular velocity \( \omega \) is related to the linear velocity \( v \) by \( \omega = \frac{v}{R} \).
Step 2: Equating energy.
Equating the potential energy to the total kinetic energy, we have:
\[
mgh = \frac{1}{2} M v^2 + \frac{1}{2} \cdot \frac{1}{2} M v^2 = \frac{3}{4} M v^2
\]
Thus,
\[
mgh = \frac{3}{4} M v^2
\]
Step 3: Solving for height.
Now, using \( mgh = Mgh \) (since the mass of the cylinder is \( M \)), we can solve for the height \( h \) as:
\[
h = \frac{3v^2}{4g}
\]
Step 4: Conclusion.
The correct answer is (A) \( \frac{3v^2}{4g} \).