A cylinder of mass m radius R is spined ...

A cylinder of mass m radius R is spined to a clockwise angular velocity `omega_(o)` and then gently placed on an inclined plane for which coefficient of friction `mu = tan theta, theta` is the angle of inclined plane with the horizontal. The centre of mass of cylinder will remain stationary for time

`omega_(o)R//g sin theta`

`2 omega)(o)R//3g sin theta`

`2 omega_(o)R//5 sin theta`

`omega_(o)R//2 g sin theta`

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