A particle of mass M and charge Q moving with a velocity →v described a circular path of radius R when subjected to a uniform transverse magnetic field of induction B. The work done by the field when the particle completes one full circle is
A
zero
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B
BQ2πR
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C
BQv(2πR)
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D
(Mv2R)(2πR)
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Solution
The correct option is Bzero →Fmag=q(→v×→B) Work done on the particle W=∫Pdt But, P=→Fmag.→v=q(→v×→B).→v=0 since →v×→B⊥→v ∴W=0. Also, one can look at it from displacement perspective. Since the particle comes back to the same position after one cycle, →ds is zero. ⇒W=0