MCQ
A planet of core density $3 \rho$ and outer crust of density $\rho$ has small tunnel in core. A small particle of mass $m$ is released from end $A$ then time required to reach end $B$
  • A
    $\sqrt {\frac{\pi }{{\rho G}}} $
  • $\frac{1}{2}\sqrt {\frac{\pi }{{\rho G}}} $
  • C
    $\pi \sqrt {\frac{1}{{\rho G}}} $
  • D
    $2\pi \sqrt {\frac{1}{{\rho G}}} $

Answer

Correct option: B.
$\frac{1}{2}\sqrt {\frac{\pi }{{\rho G}}} $
b
at some distance from centre inside core

$\mathrm{F}=-\left(\frac{G \frac{4}{3} \pi r^{3}(3 \rho) m}{r^{2}}\right)$

$\mathrm{ma}=-4 \pi G \rho m r$

$\mathrm{a}=-4 \pi G \rho r$

so $\omega=\sqrt{4 \pi G \rho}=\frac{2 \pi}{T}$

or $\mathrm{T}=2 \pi \cdot \sqrt{\frac{1}{4 \pi G \rho}}=\sqrt{\frac{\pi}{G \rho}}$

now time for $A$ to $B$ $\frac{1}{2} \sqrt{\frac{\pi}{G \rho}}$

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