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A metal rod of length L is placed normal...

A metal rod of length L is placed normal to a magnetic field and rotated through one end of rod in circular path with frequency f. The potential difference between it ends will be-

A

`piL^(2)Bf`

B

`BL//f`

C

`piL^(2)B//f`

D

fBL

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The correct Answer is:
To find the potential difference between the ends of a metal rod of length \( L \) that is rotated in a magnetic field with frequency \( f \), we can follow these steps: ### Step-by-Step Solution: 1. **Understand the Setup**: - A metal rod of length \( L \) is placed perpendicular (normal) to a magnetic field \( B \). - The rod is rotated about one of its ends in a circular path with a frequency \( f \). 2. **Identify the Formula for EMF**: - The electromotive force (emf) induced in a rotating rod in a magnetic field is given by the formula: \[ E = \frac{1}{2} B \omega L^2 \] where \( E \) is the induced emf, \( B \) is the magnetic field strength, \( \omega \) is the angular velocity, and \( L \) is the length of the rod. 3. **Convert Frequency to Angular Velocity**: - The angular velocity \( \omega \) can be related to the frequency \( f \) by the formula: \[ \omega = 2 \pi f \] 4. **Substitute \( \omega \) into the EMF Formula**: - Replace \( \omega \) in the emf formula: \[ E = \frac{1}{2} B (2 \pi f) L^2 \] 5. **Simplify the Expression**: - Simplifying the equation gives: \[ E = B \pi f L^2 \] 6. **Final Result**: - Therefore, the potential difference (emf) between the ends of the rod is: \[ E = \pi L^2 B f \] ### Conclusion: The potential difference between the ends of the rod is given by: \[ E = \pi L^2 B f \]

To find the potential difference between the ends of a metal rod of length \( L \) that is rotated in a magnetic field with frequency \( f \), we can follow these steps: ### Step-by-Step Solution: 1. **Understand the Setup**: - A metal rod of length \( L \) is placed perpendicular (normal) to a magnetic field \( B \). - The rod is rotated about one of its ends in a circular path with a frequency \( f \). ...
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