(a) $B_{A} = 0$
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$B_{B} = \ \frac{\mu_{0}}{4\pi}\frac{(2\pi - \pi/2)I\ }{r}\ \otimes = \frac{\mu_{0}}{4\pi}\ \frac{3\pi I}{2r}$
$B_{C} = \frac{\mu_{0}I}{4\pi r} \otimes \ $
So, net magnetic field at the centre
$= B_{A} + B_{B} + \ B_{C}$
$= 0 + \frac{\mu_{0}}{4\pi}\frac{3\pi I}{2r} + \frac{\mu_{0}I}{4\pi r} = \frac{\mu_{0}}{4\pi}\frac{I}{r}\left( \frac{3\pi}{2} + 1 \right)$