The correct option is B 2g3
The portion of the strings between the ceiling and the cylinder is at rest. Hence the points of the cylinder where the strings leave it are at rest. The cylinder is thus rolling without slipping on the strings.
Suppose the centre of the cylinder falls with an acceleration a. The angular acceleration of the cylinder about its axis is α=a/R, as the cylinder does not slip over the strings.
The equation of motion for the centre of mass of the cylinder is
mg−2T=ma ... (i)
For rotational motion about axis passing through C.O.M,
R×2T=I.α
where R→ radius of cylinder
⇒2TR=mR22×(aR)
⇒T=ma4 ... (ii)
From eqn. (i) and (ii)
mg−2(ma4)=ma
⇒a=2g3