The work done by a normal magnetic field in revolving a charged particle q in a circular path will be
A
zero
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B
MB(1−cosθ)
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C
MB
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D
−MB
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Solution
The correct option is B zero →Fmagnetic=q(→v×→B) ∴→Fmagnetic.→v=0 Hence, there is no power supplied to the charged particle over a cycle. ⇒ work done is zero.