The correct option is
B If
μ=tanθ, then sphere will move up the plane and frictional force acting all the time will be
2mgsinθ.
μ=tanθ is the condition for no slipping for a body placed on a rough inclined plane. Hence in this case, solid sphere will remain in translational equilbrium with friction
f balancing
mgsinθ.
τmg=0 as it passes through the centre. However due to torque provided by friction about the centre i.e
τf=fR, sphere will have angular acceleration
(α) in a direction opposite to
ω which will decrease the angular velocity
(ω) till it becomes zero. After that, it will move downwards along the inclined plane and pure rolling will start after some time due to friction coming in picture again.
Thus, option
(A) is correct and
(B) is wrong.
If
μ=tanθ2, then the sphere will slip down the inclined plane immediately, so the kinetic friction force at point of contact will act upward. Torque due to this kinetic friction will be opposite to angular velocity, so it is possible that sphere will attain angular velocity
ω′ and velocity
v′ such that
v′=ω′R i.e pure rolling.
In the case of movable inclined plane, since there is no external force on the system of (wedge+ cylinder) in
x direction, therefore linear momentum of system will remain conserved along horizontal or
x− direction.
Option
(C) is correct.