Let us consider the given diagram,
Frictional force (f) is acting in the opposite direction of F.
Now, let ‘a’ and α be the linear and angular acceleration respectively.
Let the acceleration of the centre of mass of disc be ‘a’, then
F-f = Ma .........(1)
where m is mass of disc.
Force of friction applies torque about centre.
The angular acceleration of the disc is α = a/R. (pure rolling)
Then τ = Iα or \(f\times R = (\frac{1}{2}MR^2)\times a\)
\(f \times R = (\frac{1}{2}MR^2)\frac{a}{R}\)
or Ma = 2f
F – f = 2f or F = 3f ..........(2)
from (1) and (2), we get
f ≤ μN
Thus, f = F/3.
Since there is no sliding.
or f ≤ μ mg
or F ≤ 3 μ Mg.