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The wire loop shown in the figure carries a steady current \(I\). Each straight section of the loop has length \(d\). A part of the loop lies in \(xy\) plane and the other part is tilted at 30° with respect to the \(xz\) plane. The magnitude of the magnetic dipole moment of the loop (in appropriate units) is

Loop PQRSTUP of six sides of length d: square PQRS in the xy plane with P at the origin and PQ along y, and square PSTU hinged on PS and tilted 30 degrees from the xz plane

  • A.\(\sqrt{2}Id^{2}\)
  • B.\(2 Id^{2}\)
  • C.\(\sqrt{3}Id^{2}\)
  • D.\(Id^{2}\)

Answer: D

The magnitude of the dipole moment is \(Id^{2}\).

Add and subtract the side PS (from S to P): the loop P-Q-R-S-T-U-P is then the sum of two square loops, PQRS in the \(xy\) plane and PSTU in the tilted plane, each of area \(d^{2}\), with the shared side cancelling.

PQRS, traversed P to Q (along \(+y\)) then Q to R (along \(-x\)), has moment \(Id^{2}\hat{z}\). PSTU contains PS (along \(-x\)) and PU, which leans 30° from the \(z\)-axis towards \(+y\); its moment is perpendicular to its plane:

\[ \begin{aligned} \vec{m}_{2} &= Id^{2}(\cos 30^{\circ}\hat{y} - \sin 30^{\circ}\hat{z}) \\ \vec{m} &= Id^{2}\left(\tfrac{\sqrt{3}}{2}\hat{y} + \tfrac{1}{2}\hat{z}\right) \\ |\vec{m}| &= Id^{2} \end{aligned} \]

Adding the two squares' moments as if they were perpendicular gives \(\sqrt{2}Id^{2}\), and as if parallel \(2Id^{2}\); they are in fact 120° apart, so the resultant has the magnitude of either one.

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