TS EAMCET · Physics · Rotational Motion
A thin uniform wire of mass ' \(m\) ' and linear density ' \(\rho\) ' is bent in the form of a circular ring. The moment of inertia of the ring about a tangent parallel to its diameter is
- A \(\frac{3 \mathrm{~m}^3}{8 \pi^2 \rho^2}\)
- B \(\frac{8 \mathrm{~m}^3}{3 \pi^2 \rho^2}\)
- C \(\frac{8 \pi^2 \mathrm{~m}^3}{3 \rho^2}\)
- D \(\frac{3 \pi^2 \mathrm{~m}^3}{8 \rho^2}\)
Answer & Solution
Correct Answer
(A) \(\frac{3 \mathrm{~m}^3}{8 \pi^2 \rho^2}\)
Step-by-step Solution
Detailed explanation
\(R = \frac{m}{2\pi \rho}\) \(I_{dia} = \frac{1}{2} mR^2\) \(I_{tangent} = I_{dia} + mR^2 = \frac{1}{2} mR^2 + mR^2 = \frac{3}{2} mR^2\) \(I_{tangent} = \frac{3}{2} m \left( \frac{m}{2\pi \rho} \right)^2 = \frac{3}{2} m \frac{m^2}{4\pi^2 \rho^2} = \frac{3 m^3}{8 \pi^2 \rho^2}\)
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