Step 1: Understand geometry
The rod is bent into 4 equal segments, each of length $L$ and mass $m$.
So total:
\[
\text{Length} = 4L,\quad \text{Mass} = 4m
\]
Step 2: Break into 4 rods
Each segment contributes moment of inertia about point $O$.
We use:
\[
I = I_{\text{cm}} + m d^2
\]
(Parallel axis theorem)
Step 3: Contribution of each segment
Because of symmetry:
- Two inner segments (meeting at $O$)
- Two outer segments (farther from $O$)
(i) Inner segments
Each has one end at $O$, so:
\[
I = \frac{1}{3} m L^2
\]
Two such rods:
\[
I_{\text{inner}} = 2 \times \frac{1}{3} mL^2 = \frac{2mL^2}{3}
\]
(ii) Outer segments
Each outer rod is at distance $L$ from $O$
Using parallel axis theorem:
\[
I = \frac{1}{3} mL^2 + mL^2 = \frac{4}{3} mL^2
\]
Two such rods:
\[
I_{\text{outer}} = 2 \times \frac{4}{3} mL^2 = \frac{8mL^2}{3}
\]
Step 4: Total moment of inertia
\[
I = \frac{2mL^2}{3} + \frac{8mL^2}{3}
= \frac{10mL^2}{3}
\]
Final Answer: Option (B)