A magnet of magnetic moment M is situated with its axis along the direction of a magnetic field of strength B. The work done in rotating it by an angle of 180∘ will be
A
−MB
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B
+MB
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C
0
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D
+2MB
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Solution
The correct option is D+2MB Wfield=−ΔU=Ui−Uf
U→ Magnetic potential energy.
θ→ Angle between −→M and →B
U=−−→M⋅→B
Now, initially θi=0∘
and finally θf=180∘
So,
Wfield=−MBcos0∘−(−MBcos180∘)
Wfield=−MB−MB=−2MB
Since, there is no change in kinetic energy of the system,