Calculate the magnetic field at the center due to one loop:
\[ B = \frac{\mu_0 I}{2a} \]
Since there are two loops in perpendicular planes, the resultant magnetic field is:
\[ B_{\text{net}} = \sqrt{B^2 + B^2} = \frac{\mu_0 I}{\sqrt{2}a} \]
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 the \( xy \)-plane and the other part is tilted at \( 30^\circ \) with respect to the \( xz \)-plane. The magnitude of the magnetic dipole moment of the loop (in appropriate units) is: