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A rigid circular disc of radius \(r\) (in m) is rolling without slipping on a flat surface as shown in the figure below. The angular velocity of the disc is \(\omega\) (in rad \(\text{s}^{-1}\)). The velocities (in m \(\text{s}^{-1}\)) at points \(O\) and \(A\), respectively, are

A disc of radius r with centre O touching the ground at A, rotating clockwise with angular velocity omega; unit vector i points right and j up

  • A.\(r\omega\,\hat{i}\) and \(0\,\hat{i}\)
  • B.\(-r\omega\,\hat{i}\) and \(0\,\hat{i}\)
  • C.\(-r\omega\,\hat{i}\) and \(-r\omega\,\hat{i}\)
  • D.\(r\omega\,\hat{i}\) and \(r\omega\,\hat{i}\)

Answer: A

The velocities are \(r\omega\,\hat{i}\) at O and \(0\,\hat{i}\) at A.

In rolling without slipping, the contact point A has zero velocity, because it does not slide on the ground. The disc turns clockwise, as the arrow shows, so it rolls to the right, in the \(+\hat{i}\) direction.

The centre is a distance \(r\) above the instantaneous centre A, so its speed is \(r\omega\), directed along \(+\hat{i}\). \(-r\omega\,\hat{i}\) would be anticlockwise rolling. The options giving A a velocity of \(\pm r\omega\) contradict the no-slip condition.

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