$A$ satellite is orbiting just above the surface of a planet of density $\rho$ with a periodic time $T$. The quantity $T^2 \rho$ is equal to ($G=$ universal gravitational constant).

  • A
    $\frac{4 \pi^2}{G}$
  • B
    $\frac{3 \pi^2}{G}$
  • C
    $\frac{3 \pi}{G}$
  • D
    $\frac{\pi}{G}$

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