(a) Magnetic field a $B$
$B_{1} = \frac{\mu_{0}}{2\pi}\frac{i\mathrm{\Delta}l}{r}$
Magnetic field at $A$
$B_{2} = \frac{\mu_{0}}{2\pi}\frac{i\mathrm{\Delta}l}{r}$
The resultant magnetic field at the centre
$\left| B_{A} \right| = \left| B_{B} \right|$
So, magnetic field become is zero.