Step 1: Angular motion relationship.
The wheel stops under uniform angular deceleration. \[ \omega = \omega_0 - \alpha t \] At rest, \(\omega = 0 \Rightarrow \alpha = \dfrac{\omega_0}{t_0}\).
Step 2: Use rotational kinematic equation.
\[ \theta = \omega_0 t_0 - \frac{1}{2}\alpha t_0^2 = \frac{1}{2}\omega_0 t_0 \] Since \(\omega_0 = 2\pi f_0\), number of revolutions \(N = \dfrac{\theta}{2\pi} = \dfrac{f_0 t_0}{2}\).
Step 3: Conclusion.
Hence, the wheel makes \(\dfrac{f_0 t_0}{2}\) revolutions before stopping.
A uniform rigid meter-scale is held horizontally with one of its end at the edge of a table and the other supported by hand. Some coins of negligible mass are kept on the meter scale as shown in the figure. As the hand supporting the scale is removed, the scale starts rotating about its edge on the table and the coins start moving. If a photograph of the rotating scale is taken soon after, it will look closest to: 
The angular momentum of a particle relative to the origin varies with time (\(t\)) as \(\vec{L} = (4\hat{i} + \alpha t^2 \hat{j})\, \mathrm{kg \cdot m}^2/\mathrm{s}\), where \(\alpha = 1\, \mathrm{kg \cdot m}^2/\mathrm{s}^3\). The angle between \(\vec{L}\) and the torque acting on the particle becomes \(45^\circ\) after a time of ............ s.