$A$ satellite can be in a geostationary orbit around a planet at a distance $r$ from the centre of the planet. If the angular velocity of the planet about its axis doubles,a satellite can now be in a geostationary orbit around the planet if its distance from the centre of the planet is

  • A
    $r/2$
  • B
    $r/(2\sqrt{2})$
  • C
    $r/(4^{1/3})$
  • D
    $r/(2^{1/3})$

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