A uniform magnetic field $\vec{B}$ is established along the positive z-direction. A rectangular loop of sides 'a' and 'b' carries a current of I as shown in figure. The torque in the loop is: |
IabB \((-\hat{j})\) IabB \((\hat{j})\) IabB \((\hat{k})\) IabB \((\hat{i})\) |
IabB \((\hat{j})\) |
The correct answer is Option (2) → IabB \((\hat{j})\) The loop lies in the $YZ$-plane. Current direction is clockwise when viewed from the positive $X$-axis, so by the right-hand rule, the magnetic moment is along negative $X$-direction: $\vec{m} = Iab(-\hat{i})$ Magnetic field is along positive $Z$-direction: $\vec{B} = B\hat{k}$ Torque on the loop: $\vec{\tau} = \vec{m} \times \vec{B}$ Using cross product: $\vec{\tau} = (-Iab\hat{i}) \times (B\hat{k})$ $= -IabB(\hat{i} \times \hat{k})$ Since $\hat{i} \times \hat{k} = -\hat{j}$ therefore, $\vec{\tau} = -IabB(-\hat{j})$ $\vec{\tau} = IabB\hat{j}$ So the correct answer is: $IabB(\hat{j})$
|