A heavy homogenous cylinder has mass m and radius R. It is accelerated by a force F which is applied to the cylinder. The coefficient of static friction is sufficient for the cylinder to roll without slipping then
The acceleration of the centre of the cylinder is 2F3mR(R+r)
It is possible to choose 'r' so that acceleration of centre of cylinder is greater than Fm
Let f be the frictional force: F−f=macm and Fr+fR=Iα=mR22α
For pure rolling αR=acm Hence F−fm=2(Fr+fRmR or FR-fR = 2Fr + 2fR
f=F(−2r+R)3R=2F3(−rR+12) and acm=Fm−2F3m(−rR+12)=2f3mR(3R2+r−R2)=2F3mR(R+r)
If acm>Fm;2F3mR(R+r)>Fm or 2R+2r>3R or r>R2
It is possible that am>Fm if r>R2 or For r=R2
f=2R3(12−12)=0 or if r<R2, the friction force acts in the same directionas F