The time period of oscillation of a bar magnet suspended horizontally along the magnetic meridian is $T_0$. If this magnet is replaced by another magnet of the same size and pole strength but with double the mass,the new time period will be

  • A
    $\frac{T_0}{2}$
  • B
    $\frac{T_0}{\sqrt{2}}$
  • C
    $\sqrt{2} T_0$
  • D
    $2 T_0$

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