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The length of a magnet is large compared...

The length of a magnet is large compared to its width and breadth. The time period of its oscillation in a vibration magnetometer is ` 2 s`. The magnet is cut along its length into three equal parts and these parts are then placed on each other with their like poles together . The time period of this combination will be

A

2s

B

`(2)/(3)s`

C

`2sqrt3s`

D

`(2)/(sqrt3)s`

Text Solution

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The correct Answer is:
To solve the problem, we need to analyze how the time period of oscillation of a magnet changes when it is cut and reassembled. ### Step-by-Step Solution: 1. **Understand the Initial Conditions:** - The initial time period \( T \) of the magnet is given as \( 2 \, \text{s} \). - The magnet is cut into three equal parts along its length. 2. **Determine the Moment of Inertia:** - The moment of inertia \( I \) of a uniform rod about its end is given by the formula: \[ I = \frac{1}{3} m L^2 \] - For the original magnet of mass \( M \) and length \( L \), the moment of inertia is: \[ I = \frac{1}{3} M L^2 \] 3. **Calculate the Moment of Inertia After Cutting:** - When the magnet is cut into three equal parts, each part has a mass of \( \frac{M}{3} \) and a length of \( \frac{L}{3} \). - The moment of inertia for each part about its end is: \[ I_{\text{part}} = \frac{1}{3} \left(\frac{M}{3}\right) \left(\frac{L}{3}\right)^2 = \frac{1}{3} \cdot \frac{M}{3} \cdot \frac{L^2}{9} = \frac{M L^2}{81} \] - Since there are three parts, the total moment of inertia \( I' \) of the stacked parts is: \[ I' = 3 \cdot I_{\text{part}} = 3 \cdot \frac{M L^2}{81} = \frac{M L^2}{27} \] 4. **Relate the Time Period to the Moment of Inertia:** - The time period \( T \) of a magnet in a vibration magnetometer is given by: \[ T = 2\pi \sqrt{\frac{I}{B}} \] - Since the magnetic moment \( M \) remains unchanged, we can express the new time period \( T' \) as: \[ T' = 2\pi \sqrt{\frac{I'}{B}} \] 5. **Calculate the New Time Period:** - From the relationship between the original and new moments of inertia: \[ \frac{T'}{T} = \sqrt{\frac{I'}{I}} \implies T' = T \sqrt{\frac{I'}{I}} \] - Substitute \( I' = \frac{M L^2}{27} \) and \( I = \frac{M L^2}{3} \): \[ \frac{I'}{I} = \frac{\frac{M L^2}{27}}{\frac{M L^2}{3}} = \frac{1}{9} \] - Therefore: \[ T' = T \sqrt{\frac{1}{9}} = T \cdot \frac{1}{3} \] - Since \( T = 2 \, \text{s} \): \[ T' = 2 \cdot \frac{1}{3} = \frac{2}{3} \, \text{s} \] 6. **Final Answer:** - The new time period of the combination is \( \frac{2}{3} \, \text{s} \).

To solve the problem, we need to analyze how the time period of oscillation of a magnet changes when it is cut and reassembled. ### Step-by-Step Solution: 1. **Understand the Initial Conditions:** - The initial time period \( T \) of the magnet is given as \( 2 \, \text{s} \). - The magnet is cut into three equal parts along its length. ...
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