(c) The magnetic induction due to both semicircular parts will be in the same direction perpendicular to the paper inwards
$\therefore B = B_{1} + B_{2} = \frac{\mu_{0}i}{4r_{1}} + \frac{\mu_{0}i}{4r_{2}} = \frac{\mu_{0}i}{4}\left( \frac{r_{1} + r_{2}}{r_{1}r_{2}} \right)\bigotimes$