(c) The point $P$ is lying symmetrically w.r.t. the two long straight current carrying conductors. The magnetic field at $P$ due to these current carrying conductors are mutually perpendicular.
$B_{1} = \frac{\mu_{0}}{2\pi}.\frac{i_{1}}{a}$
$B_{2} = \frac{\mu_{0}}{2\pi}.\frac{i_{2}}{a}$
$B\ \ = \ \sqrt{B_{1}^{2} + B_{2}^{2}} = \frac{\mu_{0}}{2\pi a}\ \left( i_{1}^{2} + i_{2}^{2} \right)^{1/2}$