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The time period of oscillation of a bar ...

The time period of oscillation of a bar magnet suspended horizontaliy 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

`(T_(0))/(2)`

B

`(T_(0))/(sqrt(2))`

C

`sqrt(2) T_(0)`

D

`2 T_(0)`

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The correct Answer is:
To solve the problem, we need to determine how the time period of oscillation of a bar magnet changes when its mass is doubled while keeping its size and pole strength constant. ### Step-by-Step Solution: 1. **Understand the Formula for Time Period**: The time period \( T \) of a bar magnet oscillating in a magnetic field is given by the formula: \[ T = 2\pi \sqrt{\frac{I}{M B}} \] where: - \( I \) is the moment of inertia of the magnet, - \( M \) is the mass of the magnet, - \( B \) is the magnetic field strength. 2. **Determine Moment of Inertia**: For a bar magnet, the moment of inertia \( I \) about its center is given by: \[ I = m r^2 \] where \( m \) is the mass of the magnet and \( r \) is the distance from the pivot to the center of mass. 3. **Initial Time Period**: Let the initial mass of the magnet be \( m \). The initial time period \( T_0 \) can be expressed as: \[ T_0 = 2\pi \sqrt{\frac{m r^2}{m B}} = 2\pi \sqrt{\frac{r^2}{B}} \] 4. **New Time Period with Double Mass**: When the mass is doubled (new mass \( M = 2m \)), the new moment of inertia becomes: \[ I' = 2m r^2 \] The new time period \( T' \) can be expressed as: \[ T' = 2\pi \sqrt{\frac{I'}{M' B}} = 2\pi \sqrt{\frac{2m r^2}{2m B}} = 2\pi \sqrt{\frac{r^2}{B}} \] 5. **Comparing the Two Time Periods**: Notice that the expression for \( T' \) simplifies to: \[ T' = 2\pi \sqrt{\frac{r^2}{B}} \cdot \sqrt{2} = \sqrt{2} \cdot T_0 \] Thus, the new time period \( T' \) is: \[ T' = \sqrt{2} T_0 \] ### Final Answer: The new time period will be: \[ T' = \sqrt{2} T_0 \]
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