The correct option is
C 493 NUsing Newton's 2nd Law of motion,
Mgsinθ−f=Ma ......(1) along the inclined plane where f is the frictional force up the incline.
Mgcosθ=N .........(2) perpendicular to the inclined plane.
Substituting (2) in (1) we get,
Mgsinθ−μN=Ma∴Mgsinθ−μMgcosθ=MaOnly frictional force exerts torque since weight Mg and normal reaction N pass through the centre of the cylinder and do not exert any torque.
Torque due to frictional force is
τ=fR where R is the radius of the cylinder.
Using equation for rotational motion,
τ=fR=Iα .....(3) where I is the MI of the cylinder about its center and
α is the angular acceleration.
Since there is no slipping, linear acceleration
a=RαSubstituting
a=Rα in (3) we get,
f=IαR=12MR2×aR2=Ma2 .....(4)
Substituting for Ma from eqn(1) in eqn(4)
f=Mgsinθ−f2⇒3f=Mgsinθ⇒f=Mgsinθ3=10×9.8×sin3003=493N