Method 1: Force/Torque Method:
Let `a=` linear acceleration and `alpha=` angular acceleration of the cylinder. For the linear motion of the cylinder.
`mg-2T=ma`
For the rotational motion: Net torque `=Ialpha`
Also, the linear acceleration of the cyinder is the same as the tangential acceleration of an point its surface, `a=Ralpha`
Combining the three equations, we get
`mg=ma+m/2aimpliesa=2/3g`
Method 2: Energy method
The motion of the cylinder is rotational and translation combined . Using conservation of mechanical energy
`/_K=/_U=0`
`/_K+/_U=0`
or Loss in `PE =` gain in `KE`
`mgh=1/2mv^(2)+1/2Iomega^(2)`
Constraint relation
Velocity of point `P v_(P)=0v-omegaR`
`omega=v/R` .........i
From eqn and i and ii `mgh=1/2mv^(2)+1/2((mR)/2(v/R)^(2)`
`=m/2 (v^(2)+(v^(2))/2)`
`2gh=3/2v^(2)implies v^(2)=4/3gh` ..... ii
Differentiating eqn iii with respect to time, we get
`2v(dv)/(dt)=4/3g(dh)/(dg)`
`22va=4/3gvimpliesa=2/3g`