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Question

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


A

The fractional force is 2F3

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B

The acceleration of the centre of the cylinder is 2F3mR(R+r)

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C

It is possible to choose 'r' so that acceleration of centre of cylinder is greater than Fm

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D

The direction of frictional force is always opposite to F

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Solution

The correct options are
B

The acceleration of the centre of the cylinder is 2F3mR(R+r)


C

It is possible to choose 'r' so that acceleration of centre of cylinder is greater than Fm


Let f be the frictional force: Ff=macm and Fr+fR=Iα=mR22α

For pure rolling αR=acm Hence Ffm=2(Fr+fRmR or FR-fR = 2Fr + 2fR

f=F(2r+R)3R=2F3(rR+12) and acm=Fm2F3m(rR+12)=2f3mR(3R2+rR2)=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(1212)=0 or if r<R2, the friction force acts in the same directionas F


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