A magnetic dipole placed in two perpendicular magnetic fields →B and →B∘ is in equilibrium making an angle θ with →B then
A
B=B∘
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B
Bcosθ=B∘sinθ
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C
Bsinθ=B∘cosθ
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D
B=B∘tanθ
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Solution
The correct option is CBsinθ=B∘cosθ For equilibrium of dipole net torque on the loop should be zero. So, →Z=→M×→B →Z1=→Zo →M×→B=→M×→Bo MBsinθ=MBosin(90o−θ) Bsinθ=Bocosθ(∵sin(90o−θ)=cosθ)