A block is attached to two unstretched springs and with spring constants and , respectively (see fig. I). The other ends are attached to identical supports and not attached to the walls. The springs and supports have negligible mass. There is no friction anywhere. The block is displaced towards wall 1 by a small distance (figure II) and released. The block returns and moves a maximum distance towards wall 2. Displacements and are measured with respect to the equilibrium position of the block . The ratio is -
Answer: C.
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Written solution
Step 1: Analyze the initial displacement towards Wall 1.
When the block is displaced towards Wall 1 (to the right) by a distance , support is pressed against Wall 1. Thus, spring (with spring constant ) is compressed by .
Since support is massless and free, it slides to the right by along with the block, keeping spring relaxed.
The potential energy stored in the system at this initial position is:
Step 2: Analyze the motion past the equilibrium position towards Wall 2.
Upon release, the block moves back to the equilibrium position, converting the stored potential energy into kinetic energy.
As the block continues past the equilibrium position towards Wall 2 (to the left) by a maximum distance , support is pinned against Wall 2. This causes spring (with spring constant ) to compress by .
Meanwhile, the massless support is pulled away from Wall 1 and moves freely with the block, keeping spring relaxed.
The potential energy stored in the system at the maximum displacement is:
Step 3: Apply conservation of mechanical energy.
Since there is no friction, the total mechanical energy of the system is conserved.
Simplify the equation to find the ratio of the displacements.
Answer: The ratio is (or ).