A hydrometer executes SHM when pushed into a liquid of density \( \rho \). If the mass of hydrometer is \( m \) and the radius of the tube is \( r \), then the time period of oscillation is:
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For SHM in fluids, use buoyant restoring force \( F = -\rho g A x \) and \( T = 2\pi \sqrt{\frac{m}{k}} \).
\( T = \frac{1}{2\pi} \sqrt{\frac{m}{\pi r^2 \rho g}} \)
\( T = \frac{1}{2\pi} \sqrt{\frac{\pi r^2 \rho g}{m}} \)
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The Correct Option isA
Solution and Explanation
Restoring force due to buoyancy: \( F = \rho g A x \), where \( A = \pi r^2 \).
\[
F = -\rho g \pi r^2 x \Rightarrow F = -k x \Rightarrow k = \rho g \pi r^2
\]
Now, time period of SHM is:
\[
T = 2\pi \sqrt{\frac{m}{k}} = 2\pi \sqrt{\frac{m}{\rho g \pi r^2}}
\]