To determine which object, the disk or the sphere, reaches the bottom of the inclined plane first, we need to consider the physics of rolling motion and energy conservation.
- Concept of Rolling Motion: Both the disk and the sphere roll without slipping. This means the motion includes both translational and rotational components.
- Energy Conservation during Rolling: The potential energy at the top of the incline is converted into translational and rotational kinetic energy at the bottom.
- The total mechanical energy at the top is given by:
\(E_{\text{initial}} = mgh\), where \(m\) is the mass, \(g\) is gravity, and \(h\) is the height. - At the bottom of the incline, the energy is:
\(E_{\text{final}} = \frac{1}{2}mv^2 + \frac{1}{2}I\omega^2\), where \(v\) is the linear velocity and \(I\omega^2\) is the rotational kinetic energy. Here, \(I\) is the moment of inertia and \(\omega\) is the angular velocity.
- Moment of Inertia:
- For a disk, \(I_{\text{disk}} = \frac{1}{2}mr^2\)
- For a sphere, \(I_{\text{sphere}} = \frac{2}{5}mr^2\)
- Roll Dynamics and Acceleration:
- Acceleration \(a\) of a rolling object down an incline is proportional to \(\frac{g \sin \theta}{1 + \frac{I}{mr^2}}\).
- Thus, \(a_{\text{disk}} = \frac{g \sin \theta}{1 + \frac{1}{2}}\) and \(a_{\text{sphere}} = \frac{g \sin \theta}{1 + \frac{2}{5}}\).
- Conclusion: Due to its smaller moment of inertia, for the same translational and rotational energy distribution, the sphere accelerates faster and will reach the bottom of the incline first.
Answer: Sphere