(d) Magnetic field at $O\ due\ to\ PR$
$B_{1} = \frac{\mu_{0}}{4\pi}\ \frac{2i/3}{r}$ $\lbrack\sin{30{^\circ} + \sin{30{^\circ}\rbrack\ }}$
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$\ = \frac{\mu_{0}}{4\pi}\frac{2i}{3r}$
It is directed outside the paper. Magnetic field at $O,$ due to $PQR$,
$B_{2}\ \ = 2 \times \frac{\mu_{0}}{4\pi}\ \frac{(i/3)}{\mu}\ \lbrack\sin{30{^\circ} + \sin{30{^\circ}\rbrack}}$
$\ \ $= $\frac{\mu_{0}}{4\pi}\frac{2i}{3r}$
It is directed inside the paper.
$\therefore\ \ \ \ $Resultant magnetic field at $O,$
$B = B_{1} - B_{2} =$0