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Asked in GUJCET 2011 · Dipole in a uniform field
Given: the magnet starts in stable equilibrium, so ⃗M is along ⃗B and θ₁=0°; it is turned to θ₂=180°.
Idea: the potential energy of a dipole in a uniform field is U=-MB cos θ, and the work done in turning it is the rise in this energy, W=U₂-U₁=MB(cos θ₁-cos θ₂).
W=MB(cos 0°-cos 180°)=MB(1-(-1)).
W=2MB.
The magnet is left antiparallel to ⃗B, in unstable equilibrium - the highest-energy orientation, U=+MB, reached from the lowest, U=-MB.
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