Shown in the figure is a conductor carrying a current $I$. The magnetic field intensity at the point $O$ (common centre of all the three arcs) is
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since, magnetic field at the centre of an $arc$ is equal to

$\mathrm{B}=\frac{\mu_{0} \mathrm{I}}{4 \pi \mathrm{r}} \theta$

Net $B=\frac{\mu_{0} I}{4 \pi}\left[\frac{1}{r}-\frac{1}{2 r}+\frac{1}{3 r}\right] \theta=\frac{5 \mu_{0} I \theta}{24 \pi r}$

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