A uniform disc of mass 'm' and radius R is rolling down a fixed inclined plane without slipping. The angular acceleration of the disc is
We know that ,
acm = gsingθ1+K2R2 = 12
For disc, I = MR22 = MK2
⇒ K2R2 = 12
⇒ acm = gsinθ1+12 = 23 g sin θ
∴ Angular acceleration , α = acmR [ ∴ For pure rolling , acm = r α ]
⇒ α = 2gsinθ3R