The time period \( T \) of a simple harmonic motion of a bar magnet in the Earth's magnetic field is given by the equation:
\[ T = 2\pi \sqrt{\frac{I}{mB}} \]
where \( I \) is the moment of inertia of the magnet, \( m \) is the magnetic moment, and \( B \) is the magnetic field strength.
Assuming the bar magnet is a uniform rod, we have:
\[ I = \frac{1}{12} ML^2 \]
where \( M \) is the mass of the magnet and \( L \) is its length.
If the mass \( M \) is increased by 9 times, the new moment of inertia \( I' \) becomes:
\[ I' = \frac{1}{12} (9M)L^2 = 9 \left(\frac{1}{12} ML^2 \right) = 9I \]
The new time period \( T' \) is:
\[ T' = 2\pi \sqrt{\frac{I'}{mB}} = 2\pi \sqrt{\frac{9I}{mB}} = 2\pi \cdot 3 \cdot \sqrt{\frac{I}{mB}} = 3 \cdot 2\pi \sqrt{\frac{I}{mB}} = 3T \]
Thus, the time period becomes \( 3T \) when the mass of the bar magnet is increased by 9 times.
The correct option is \( 3T \).