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The period of oscillation of a suspended...

The period of oscillation of a suspended thin cylindrical magnet is 4 seconds. It is broken into exactly two halves. Find the period of oscillation of each half when freely suspended.

A

4s

B

2s

C

1s

D

`2sqrt2s`

Text Solution

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The correct Answer is:
To find the period of oscillation of each half of a cylindrical magnet after it has been broken into two equal halves, we can follow these steps: ### Step 1: Understand the formula for the period of oscillation The period of oscillation \( T \) of a magnet can be expressed using the formula: \[ T = 2\pi \sqrt{\frac{I}{MB}} \] where: - \( I \) is the moment of inertia of the magnet, - \( M \) is the magnetic moment, - \( B \) is the magnetic field. ### Step 2: Identify the initial conditions We know that the original period of oscillation of the thin cylindrical magnet is \( T = 4 \) seconds. ### Step 3: Break the magnet into two halves When the magnet is broken into two equal halves: - The mass of each half becomes \( \frac{M}{2} \) (where \( M \) is the original mass). - The length of each half becomes \( \frac{L}{2} \) (where \( L \) is the original length). ### Step 4: Calculate the new magnetic moment for each half The magnetic moment \( M' \) for each half can be calculated as: \[ M' = \text{pole strength} \times \text{distance between poles} = \frac{M}{2} \times \frac{L}{2} = \frac{ML}{4} \] ### Step 5: Calculate the moment of inertia for each half The moment of inertia \( I' \) for each half can be calculated using the formula for a thin rod: \[ I' = \frac{1}{3} m l^2 \] Substituting \( m = \frac{M}{2} \) and \( l = \frac{L}{2} \): \[ I' = \frac{1}{3} \left(\frac{M}{2}\right) \left(\frac{L}{2}\right)^2 = \frac{1}{3} \left(\frac{M}{2}\right) \left(\frac{L^2}{4}\right) = \frac{ML^2}{24} \] ### Step 6: Substitute the new values into the period formula Now we substitute \( I' \) and \( M' \) into the period formula: \[ T' = 2\pi \sqrt{\frac{I'}{M'B}} = 2\pi \sqrt{\frac{\frac{ML^2}{24}}{\frac{ML}{4}B}} \] This simplifies to: \[ T' = 2\pi \sqrt{\frac{ML^2}{24} \cdot \frac{4}{MLB}} = 2\pi \sqrt{\frac{4L}{24B}} = 2\pi \sqrt{\frac{L}{6B}} \] ### Step 7: Relate the new period to the original period Since the original period \( T = 2\pi \sqrt{\frac{L}{MB}} \), we can relate the two periods: \[ T' = \frac{T}{\sqrt{2}} = \frac{4}{\sqrt{2}} = 2\sqrt{2} \text{ seconds} \] ### Step 8: Calculate the final result Given that \( T = 4 \) seconds, we find: \[ T' = 2 \text{ seconds} \] Thus, the period of oscillation of each half when freely suspended is **2 seconds**. ---
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