The force
F acting at the centre of the disc will produce zero torque about centre. However, force
F acting at the topmost point of the disc will tend to make it rotate in clockwise direction.
Hence, friction will act towards left at the bottom to oppose the tendency of slipping. Let
f be the friction force acting on the disc.
Applying Newton's
2nd law on the disc,
⇒2F−f=ma ...(i) Applying equation of torque about the centre of the disc,
τcom=Icom×α where
τcom= Net torque about centre of mass of the disc.
⇒τN+τmg+(τF)1+(τF)2+τf=Iα ⇒0+0+FR+0+fR=Iα [
τN=τmg=0 because
N and
mg pass through COM.
Both
F and
f are tending to rotate disc in clockwise direction, hence the torque will add.]
⇒(F+f)R=Iα ...(ii) a=Rα, condition for pure rolling
& I=mR22 Substituting in Eq.
(ii),
(F+f)R=mR22×aR ∴F+f=ma2...(iii) Adding Eq.
(i) & (iii), we get
f=0 Hence according to question,
f=nF or
0=nF ∴n=0