JEE Challenger
More from Oscillations

Ratio of Displacements for Block Connected to Springs with Unattached Supports

A block (B) is attached to two unstretched springs S1 and S2 with spring constants kk and 4 k4\ k, respectively (see figure I). The other ends are attached to identical supports M1 and M2 not attached to the walls. The springs and supports have negligible mass. There is no friction anywhere. The block B is displaced towards wall 1 by a small distance xx (figure II) and released. The block returns and moves a maximum distance yy towards wall 2. Displacements xx and yy are measured with respect to the equilibrium position of the block B. The ratio yx\frac{y}{x} is

Diagram 0

Options

A

4

B

2

C

12\frac{1}{2}

Correct
D

14\frac{1}{4}

Step-by-Step Solution

To find the ratio of the displacements yx\frac{y}{x}, we analyze the mechanical energy of the system at the two extreme positions using the Principle of Conservation of Mechanical Energy.

1. Initial State (Displacement xx towards Wall 1):

  • When the block BB is displaced to the right by a distance xx towards Wall 1:
    • Support M1M_1 rests against Wall 1, preventing further movement to the right. Thus, spring S1S_1 (with spring constant k1=kk_1 = k) is compressed by a distance xx.
    • Support M2M_2 is not attached to Wall 2, so as the block moves right, M2M_2 simply slides to the right. Spring S2S_2 (with spring constant k2=4kk_2 = 4k) remains at its relaxed (natural) length.
  • Since the block is released from rest, the initial mechanical energy of the system is entirely potential energy stored in spring S1S_1:
    Ei=12kx2E_i = \frac{1}{2} k x^2

2. Motion towards Wall 2 (Displacement yy towards Wall 2):

  • Upon release, spring S1S_1 pushes the block back towards the equilibrium position (x=0x = 0). At x=0x = 0, spring S1S_1 reaches its natural length, and support M2M_2 makes contact with Wall 2.
  • As the block continues moving to the left beyond the equilibrium position by a maximum distance yy:
    • Support M2M_2 is pressed against Wall 2 and cannot move further left, causing spring S2S_2 to be compressed by distance yy.
    • Support M1M_1 is not attached to Wall 1, so it detaches from Wall 1 and moves along with the block to the left. As a result, spring S1S_1 remains at its natural length and stores zero potential energy.
  • At the maximum displacement yy, the block momentarily comes to rest. The final mechanical energy of the system is entirely potential energy stored in spring S2S_2:
    Ef=12(4k)y2E_f = \frac{1}{2} (4k) y^2

3. Conservation of Energy:

Since all surfaces are frictionless and the springs/supports are massless, the total mechanical energy is conserved (Ei=EfE_i = E_f):

12kx2=12(4k)y2\frac{1}{2} k x^2 = \frac{1}{2} (4k) y^2

kx2=4ky2k x^2 = 4k y^2

y2x2=14\frac{y^2}{x^2} = \frac{1}{4}

Taking the square root on both sides:

yx=12\frac{y}{x} = \frac{1}{2}

Thus, the correct option is (C).