(d) Perpendicular to $O\ \ from\ PQ.$
Or $QR,\ \ a = r\sin{\theta/2}$
Magnetic field induction at $O$ due to current through $PQ\ \ and\ QR$ is
$B = \frac{\mu_{0}}{4\pi}\frac{i}{a}\ \lbrack\sin(90{^\circ} - \theta/2$)+ sin$90{^\circ}\rbrack\ \times 2\ $
$= \frac{\mu_{0}}{2\pi}\ \frac{i}{\sin{\theta/2}}(\cos{\theta/2 + 1) = \frac{\mu_{0}}{2\pi}\frac{i}{r}\ \frac{(1 + \cos{\theta/2)}}{\sin{\theta/2}}}$