The time period of oscillation of a magnetic dipole (bar magnet) in a uniform magnetic field is given by:
\[
T = 2\pi \sqrt{\frac{I}{MB}}
\]
Where:
- \( I \) is the moment of inertia of the magnet,
- \( M \) is the magnetic moment,
- \( B \) is the magnetic field strength.
For a uniform bar magnet:
\[
I \propto m \quad \text{(as the shape remains unchanged)}
\]
If the mass is quadrupled, \( m \rightarrow 4m \Rightarrow I \rightarrow 4I \)
Hence, the new time period \( T' \) becomes:
\[
T' = 2\pi \sqrt{\frac{4I}{MB}} = 2 \cdot T
\]
So, time period becomes twice, and motion remains simple harmonic.