The correct option is B
√3 W
Energy required to rotate the magnet by θ from equilibrium state is given by,
W=MB(1−cosθ)
And, when the magnet is at an orientation θ with the direction of field, torque applied on it by the field
→τ=|−→M×→B|=MBsinθ
So, we need to apply an equal but opposite torque MBsinθ to hold it in the new state.
Thus, the required torque is given by,
τreq=MB sinθ=MBsin60∘
τreq=√3MB2
Given that, W=MB(1−cos60∘)
W=(MB2)
So, τreq=√3(MB2)=√3 W
Hence, option (B) is the correct answer.