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).
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,



What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)