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Question

If a bar magnet of magnetic moment M is freely suspended in a uniform magnetic field of strength B, the work done in rotating the magnet through an angle θ is

A
MB(1sinθ)
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B
MBsin θ
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C
MBcosθ
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D
MB(1cos θ)
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Solution

The correct option is D MB(1cos θ)
We know that,

Wfield=ΔU

Wfield=UiUf

U= Magnetic potential energy of dipole in external field, which is given by,

U=M.B

Initially the magnet is alligned to field,
so that angle θ between
M and B=0

Ui=MBcos 0=MB

Finally, θf=θUf=MBcosθ

So Wfield=M B(MBcosθ)

=MB(cosθ1)

Since, there is no change in kinetic energy,

Wext=Wfield=MB(1cos θ)

Hence, option (D) is the correct answer.
Why this Question?
Tip: The work done by conservative forces and the change in potential energy of the system is related by,

Wcons=ΔU

Also,

If there is no change in the kinetic energy of the system,

Wext=Wcons

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