To solve the problem of finding the moment of inertia of a ring formed from a rod, we start with understanding the distribution of mass and geometry:
Thus, the moment of inertia of the ring about any of its diameters is \(\frac{\lambda L^3}{8\pi^2}\), which corresponds to the correct answer.
For a rod of length \( L \) and linear mass density \( \lambda \),
the total mass \( m \) of the rod is: \( m = \lambda L \)
When the rod is bent into a ring of radius \( R \), the mass is uniformly distributed along the circumference of the ring.
The moment of inertia of the ring about any of its diameters is given by the formula for a ring: \( I = \frac{1}{2} m R^2 \)
Substituting
\( m = \lambda L \) into this expression: \( I = \frac{1}{2} \lambda L R^2 \)
We know that the circumference of the ring is \( 2\pi R \), and the length of the rod is equal to the circumference of the ring, so: \( L = 2\pi R \)
Thus, the radius \( R \) can be written as: \( R = \frac{L}{2\pi} \)
Substituting this into the equation for the moment of inertia: \( I = \frac{1}{2} \lambda L \left( \frac{L}{2\pi} \right)^2 = \frac{1}{2} \lambda L \times \frac{L^2}{4\pi^2} \)
Simplifying:
\( I = \frac{\lambda L^3}{8\pi^2} \)
Thus, the moment of inertia of the ring about any of its diameters is \( \frac{\lambda L^3}{8\pi^2} \).
Therefore, the correct answer is Option (1).
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