Question:

A thin rod of length ' $4L$ ' and mass ' $4m$ ' is bent as shown. Find the moment of inertia about an axis through $O$ and perpendicular to the plane.

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Shortcut: Divide bent rod into straight segments and apply parallel axis theorem carefully.
Updated On: May 8, 2026
  • $\frac{mL^2}{3}$
  • $\frac{10mL^2}{3}$
  • $\frac{mL^2}{12}$
  • $\frac{mL^2}{24}$
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The Correct Option is B

Solution and Explanation



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)
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