(d) Considering the larger loop to be made up of four rods each of length $L$, the field at the centre,
$i.e.,$ at a distance $\left( \frac{L}{2} \right)$from each rod, will be
[image:6_image65.emf]
$B = 4 \times \frac{\mu_{0}}{4\pi}\frac{l}{d}\left\lbrack \sin\alpha + \sin\beta \right\rbrack$
$ie,\ \ \ \ B = 4 \times \frac{\mu_{0}}{4\pi}\frac{I}{\left( \frac{L}{2} \right)} \times 2\sin{45{^\circ}}$
$ie,\ \ \ \ B_{1} = \frac{\mu_{0}}{4\pi}\frac{8\sqrt{2}}{L}I$
So, the flux with smaller loop
$\ \ \ \ \ \ \ \ \ \ \phi = B_{1}S_{2} = \frac{\mu_{0}}{4\pi}\frac{8\sqrt{2}}{L}l^{2}I$
and hence, $M = \frac{\phi_{2}}{I} = 2\sqrt{2}\frac{\mu_{0}}{\pi}\frac{l^{2}}{L}$
or $\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ M \propto \frac{l^{2}}{L}$