Answer:
Option B
Explanation:
For the mass m, mg-T=ma
As we know, a= Rα
So, $mg-T=mR\alpha$ .............(i)
Torque about centre of pully
$T \times R=mR^{2}\alpha$ .........(ii)
From Eqs.(i) and (ii) , we get
$a=\frac{g}{2}$
Hence, the acceleration with the mass of a body fall is $\frac{g}{2}$