If we let c stand for the term in front of the mR2 for the various moments of inertia (c= 1 for hoop, 1/2 for cylinder, and 2/5 for a sphere), we can use energy conservation to solve for final velocity:
mgh at the top = 1/2 mv2 + 1/2 Iω2 at the bottom of the ramp
Since ω = v/R for a non-slipping rolling object, and I = cmR2 we obtain
mgh = 1/2 (1+c) mv2
which you can solve for v. Note that the mass AND the radius of the rolling object has no effect on the final velocity (only the shape has an impact)
You actually don't have to do the calculation because, the one with the most rotational inertia will go slower.
Good luck