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.
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.
