JEE Challenger
More from Mechanical Properties of Fluids

Solid Spheres Connected by Spring Submerged in Liquid Equilibrium

A solid sphere having radius RR and density ρ\rho is attached to one end of a massless spring with force constant kk. The opposite end of the spring is attached to a second solid sphere with radius RR and density 3ρ3\rho. The entire assembly is immersed in a liquid of density 2ρ2\rho and allowed to attain equilibrium. Which of the following statement(s) is/are correct?

Options

A

the net spring elongation equals 4πR3ρg3k\frac{4\pi R^3 \rho g}{3k}

Correct
B

the net spring elongation equals 8πR3ρg3k\frac{8\pi R^3 \rho g}{3k}

C

the lighter sphere remains partially submerged

D

the lighter sphere becomes fully submerged

Correct

Step-by-Step Solution

To determine the correct statement(s), let us analyze the forces acting on the two spheres in liquid equilibrium.

1. System Parameters

  • Volume of each solid sphere of radius RR: V=43πR3V = \frac{4}{3}\pi R^3
  • Mass of the lighter sphere (density ρ\rho): m1=Vρ=43πR3ρm_1 = V\rho = \frac{4}{3}\pi R^3 \rho
  • Mass of the heavier sphere (density 3ρ3\rho): m2=V(3ρ)=4πR3ρm_2 = V(3\rho) = 4\pi R^3 \rho
  • Density of the liquid: ρL=2ρ\rho_L = 2\rho

2. Overall Equilibrium of the System

The total weight of the system consisting of both spheres is: Wtotal=m1g+m2g=Vρg+3Vρg=4VρgW_{\text{total}} = m_1 g + m_2 g = V\rho g + 3V\rho g = 4V\rho g

If both spheres are completely submerged, the maximum total buoyant force exerted by the liquid is: FB,max=VρLg+VρLg=V(2ρ)g+V(2ρ)g=4VρgF_{B,\text{max}} = V \rho_L g + V \rho_L g = V(2\rho)g + V(2\rho)g = 4V\rho g

Since Wtotal=FB,maxW_{\text{total}} = F_{B,\text{max}}, the system achieves equilibrium when both spheres are completely submerged in the liquid.

If the lighter sphere were only partially submerged (say, a fraction f<1f < 1), the total buoyant force would be: FB=fV(2ρ)g+V(2ρ)g=(2f+2)VρgF_B = f V(2\rho)g + V(2\rho)g = (2f + 2)V\rho g

Setting FB=WtotalF_B = W_{\text{total}} gives: (2f+2)Vρg=4Vρg  ⟹  2f+2=4  ⟹  f=1(2f + 2)V\rho g = 4V\rho g \implies 2f + 2 = 4 \implies f = 1

Thus, the lighter sphere must be completely submerged in equilibrium. Therefore, Option (D) is correct and Option (C) is incorrect.


3. Spring Elongation

Since the density of the lighter sphere (ρ\rho) is less than that of the liquid (2ρ2\rho), it tends to float to the top. Conversely, the heavier sphere (3ρ3\rho) tends to sink to the bottom. As a result, the spring between them is in a state of extension (elongation xx).

Considering the equilibrium of the heavier sphere (bottom sphere):

  1. Downward gravitational force: W2=m2g=3VρgW_2 = m_2 g = 3V\rho g
  2. Upward buoyant force: FB2=VρLg=2VρgF_{B2} = V\rho_L g = 2V\rho g
  3. Upward spring force: Fs=kxF_s = kx

For equilibrium of the heavier sphere: FB2+Fs=W2F_{B2} + F_s = W_2 2Vρg+kx=3Vρg2V\rho g + kx = 3V\rho g kx=Vρgkx = V\rho g

Substituting V=43πR3V = \frac{4}{3}\pi R^3: kx=43πR3ρg  ⟹  x=4πR3ρg3kkx = \frac{4}{3}\pi R^3 \rho g \implies x = \frac{4\pi R^3 \rho g}{3k}

This matches Option (A).


Conclusion

  • Option (A) is correct.
  • Option (D) is correct.