(a) Magnetic field due to one side of the square at centre $O$
$B_{1} = \frac{\mu_{0}}{4\pi}.\frac{2i\sin{45{^\circ}}}{a/2} \Rightarrow B_{1} = \frac{\mu_{0}}{4\pi}.\frac{2\sqrt{2}i}{a}$
Hence magnetic field at centre due to all sides
$B = 4B_{1} = \frac{\mu_{0}(2\sqrt{2}i)}{\pi a}$
Magnetic field due to $n$ turns
$B_{net} = nB = \frac{\mu_{0}2\sqrt{2}ni}{\pi a} = \frac{\mu_{0}2\sqrt{2}ni}{\pi(2l)} = \frac{\sqrt{2}\mu_{0}ni}{\pi l}\ (\because a = 2l)$