If a bar magnet in magnetic moment m is deflected from an angle θ in a uniform magnetic field of induction B, the work done in reversing the direction is
MBsinθ
MB
MB(1−cosθ)
MBcosθ
A
MB(1−cosθ)
B
MBcosθ
C
MBsinθ
D
MB
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Solution
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Now lets assume that the bar magnetic is initially placed parallel to the field the initial potential energy will be Ui=−−→M.→B=−MBcos0=−MB Now when it is deflected by an angle θ then Uf=−−→M.→B=−MBcosθ Now we know that the work done = −ΔU ΔU=Ui−Uf ΔU=−MB(1−cosθ)
therefore, work done =MB(1−cosθ).
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