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NEET PHYSICSMedium

A rectangular block of mass mm and area of cross-section AA floats in a liquid of density ρ\rho. If it is given a small vertical displacement from equilibrium, it undergoes oscillation with a time period TT. Then:

A

TρT \propto \sqrt{\rho}

B

T1AT \propto \frac{1}{\sqrt{A}}

C

T1ρT \propto \frac{1}{\rho}

D

T1mT \propto \frac{1}{\sqrt{m}}

Step-by-Step Solution

  1. Identify the Restoring Force: When the block is depressed by a small distance xx, an additional volume of liquid V=AxV = Ax is displaced. According to Archimedes' Principle, this creates an additional upthrust (buoyant force) which acts as the restoring force. Frestoring=(Weight of displaced liquid)=(Axρ)gF_{restoring} = -(\text{Weight of displaced liquid}) = -(Ax\rho)g
  2. Determine Spring Constant (kk): Comparing this to the standard SHM equation F=kxF = -kx, we identify the effective force constant k=Aρgk = A\rho g.
  3. Apply Time Period Formula: The time period of a particle/body in SHM is given by T=2πmkT = 2\pi \sqrt{\frac{m}{k}} . Substituting k=Aρgk = A\rho g: T=2πmAρgT = 2\pi \sqrt{\frac{m}{A\rho g}}
  4. Analyze Proportionality: From the derived formula, the relationship between time period TT and cross-sectional area AA is: T1AT \propto \frac{1}{\sqrt{A}} (Note: It is also proportional to m\sqrt{m} and inversely proportional to ρ\sqrt{\rho}).
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