Step 1: Understanding the Concept:
The system undergoes a series of harmonic motions and elastic collisions. Because the masses are equal, they perfectly exchange velocities during elastic collisions.
Step 2: Detailed Explanation:
1. Sequence of Motion:
$\bullet$ Cube is released from \( x = -\ell \). It reaches \( x = 0 \) in time \( t_{1} = \frac{\pi}{2\omega} \).
$\bullet$ At \( x=0 \), it has max speed \( v = \omega \ell \). It hits the stationary sphere.
$\bullet$ Velocity exchange: Cube stops, sphere moves right with speed \( \omega \ell \).
$\bullet$ Sphere travels distance \( D \) to the wall and back. Time taken: \( t_{2} = \frac{2D}{\omega \ell} \).
$\bullet$ Sphere hits stationary cube at \( x=0 \). Velocity exchange: Sphere stops, cube moves left with \( \omega \ell \).
$\bullet$ Cube returns to \( x = -\ell \) in time \( t_{3} = \frac{\pi}{2\omega} \).
2. Total Time Period:
\[ T = \frac{\pi}{\omega} + \frac{2D}{\omega \ell} \]
3. Dependence on \( \ell \):
As \( \ell \) increases, the term \( \frac{2D}{\omega \ell} \) decreases while \( \frac{\pi}{\omega} \) remains constant. Therefore, the total period \( T \) decreases.
Step 3: Final Answer:
Increasing the initial compression \( \ell \) leads to a decrease in the time period T.