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Question
A rectangular loop of sides a and b carrying current I is placed in a magnetic field `vec B` such that its area vector `vec A` makes an angle θ with `vec B`. With the help of a suitable diagram, show that the torque `vec tau` acting on the loop is given by `vec tau = vec m xx vec B`, where `vec m(= I vec A)` is the magnetic dipole moment of the loop.
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Solution
A current-carrying loop in a magnetic field experiences torque due to magnetic forces on its sides.
Magnetic force on a current element:
`vec F = I(vec l xx vec B)`
Magnitude of force for side of length a:
F = IaB sin θ
Torque = force × perpendicular distance between forces
τ = F × b
= (IaB sin θ)b
= IabB sin θ ...[Since Area of rectangular loop (A) = ab]
= IAB sin θ
Magnetic dipole moment of loop `(vec m) = I vec A`
So the magnitude of torque (τ) = mB sin θ
The direction of torque is perpendicular to both `vec m` and `vec B`.
Thus:
`vec tau = vec m xx vec B`
