Concept:
Current divides inversely proportional to resistance.
Magnetic field at the centre due to a semicircular arc is
\[
B=\frac{\mu_0 I}{4r}
\]
Step 1: Find current division
Let resistance of arc \(ADC=R\).
Then
\[
R_{ABC}=\frac{R}{2}
\]
Current through \(ABC\),
\[
I_{ABC}
=
I_0
\frac{R}{R+\frac{R}{2}}
=
\frac{2I_0}{3}
\]
Current through \(ADC\),
\[
I_{ADC}
=
I_0
\frac{\frac{R}{2}}{R+\frac{R}{2}}
=
\frac{I_0}{3}
\]
Step 2: Find magnetic fields due to both arcs
\[
B_1
=
\frac{\mu_0}{4r}
\left(
\frac{2I_0}{3}
\right)
\]
\[
B_1
=
\frac{\mu_0 I_0}{6r}
\]
Similarly,
\[
B_2
=
\frac{\mu_0}{4r}
\left(
\frac{I_0}{3}
\right)
\]
\[
B_2
=
\frac{\mu_0 I_0}{12r}
\]
Step 3: Determine resultant field
The currents flow through opposite semicircular paths.
Hence fields are opposite.
\[
B=B_1-B_2
\]
\[
B=
\frac{\mu_0 I_0}{6r}
-
\frac{\mu_0 I_0}{12r}
\]
\[
B=
\frac{\mu_0 I_0}{12r}
\]
\[
\boxed{B=\frac{\mu_0 I_0}{12r}}
\]
Therefore,
\[
\boxed{\text{Option (C)}}
\]