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JEE Advanced 2025 Paper 1 · Physics · Fluid Mechanics, Elasticity and Surface Tension · hard

A uniform cube of side 10 cm and density 900 kg m^-3 floats in a tank with its faces horizontal and vertical, partly in water (density 1000 kg m^-3)…

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A uniform cube of side 10 cm10\ \mathrm{cm} and density 900 kg m−3900\ \mathrm{kg\,m^{-3}} floats in a tank with its faces horizontal and vertical, partly in water (density 1000 kg m−31000\ \mathrm{kg\,m^{-3}}) and partly in a layer of oil (density 800 kg m−3800\ \mathrm{kg\,m^{-3}}) lying on top of the water, the oil layer being thick enough that the cube always remains completely immersed in the two liquids. The cube is pushed slightly down along the vertical and released. Take g=10 m s−2g=10\ \mathrm{m\,s^{-2}} and neglect viscosity and surface effects. The time period of the small vertical oscillations is closest to
  1. A. 0.60 s0.60\ \mathrm{s}
  2. B. 0.67 s0.67\ \mathrm{s}
  3. C. 1.33 s1.33\ \mathrm{s}
  4. D. 0.63 s0.63\ \mathrm{s}
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Answer: (C) 1.33 s1.33\ \mathrm{s}

First find the equilibrium: if a depth xx of the cube lies in water, 900a=1000x+800(a−x)900a=1000x+800(a-x), so x=a/2x=a/2. Displace the cube down by yy: a length yy of oil is replaced by water, so the buoyant force increases by (ρw−ρo)gAy(\rho_w-\rho_o)gAy with A=a2A=a^2. The restoring force is therefore F=−(ρw−ρo)gA yF=-(\rho_w-\rho_o)gA\,y and the mass is m=ρAam=\rho Aa. Hence ω2=(ρw−ρo)gρa=200×10900×0.1=2009\omega^2=\dfrac{(\rho_w-\rho_o)g}{\rho a}=\dfrac{200\times10}{900\times0.1}=\dfrac{200}{9} and T=2π/ω=2π0.045=1.33 sT=2\pi/\omega=2\pi\sqrt{0.045}=1.33\ \mathrm{s}. Taking the cube as floating only in water gives 0.60 s0.60\ \mathrm{s}, only in oil 0.67 s0.67\ \mathrm{s}, and using the average liquid density gives 0.63 s0.63\ \mathrm{s}. All these ignore that the restoring force depends on the density difference.
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