MHT CET · Physics · Rotational Motion

Three points masses, each of mass 'm' are placed at the corners of an equilateral triangle of side \(\ell^{\prime}\). The moment of inertia of the system about an axis passing through one of the vertices and parallel to the side joining other two vertices, will be

A \(\frac{3}{2} \mathrm{~m} \ell^{2}\)
B \(\frac{3}{4} \mathrm{~m} \ell^{2}\)
C \(\frac{1}{2} \mathrm{~m} \ell^{2}\)
D \(\frac{1}{4} \mathrm{~m} \ell^{2}\)

Verified Solution

Answer & Solution

Correct Answer

(A) \(\frac{3}{2} \mathrm{~m} \ell^{2}\)

Step-by-step Solution

Detailed explanation

\(I =2 \mathrm{mh}^{2}\)
\(\mathrm{h}=\ell \sin 60^{\circ}=\ell \times \frac{\sqrt{3}}{2}\)
\(I =2 \mathrm{~m} \times \frac{3}{4} \cdot \ell^{2}=\frac{3}{2} \mathrm{~m} \ell^{2}\)

Apply the relevant identity from the chapter and substitute the values established in the previous step, keeping the original constraint in view.

Use the simplified expression to isolate the unknown, then plug the result back into the question setup to confirm the working is internally consistent.

Cross-check against a boundary or limiting case. Both the dimensional balance and the qualitative behaviour at the extreme should agree with the candidate answer.

Combine the steps above to identify the correct option. The remaining choices each fail at least one of the consistency, dimensional, or boundary checks.

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