(b) Magnetic field at the centre due to one side
$B_{1} = \frac{\mu_{0}}{4\pi}.\frac{2i\sin\theta}{r},$ where $r = a\cos\theta$
So $B_{1} = \frac{\mu_{0}}{4\pi}.\frac{2i\sin\theta}{a\cos\theta} = \frac{\mu_{0}i}{2\pi a}\tan\theta$
Hence net magnetic field
$B_{net} = n \times \frac{\mu_{0}i}{2\pi a}\tan\frac{\pi}{n}$