The moment of inertia of a solid disc about an axis passing through its center and perpendicular to its plane is given by $I = \frac{1}{2}MR^2$, where $M$ is the mass of the disc and $R$ is its radius.
Since both discs are made of iron and have negligible thickness, their mass depends on their area. For a disc, $\text{Area} = \pi R^2$. Thus the mass is proportional to $R^2$: $M \propto R^2$.
Substituting this proportionality into the moment of inertia formula: $I = \frac{1}{2}MR^2 \implies I \propto R^2 \times R^2 \implies I \propto R^4$.
Therefore, $\frac{I_2}{I_1} = \left(\frac{R_2}{R_1}\right)^4$. Given $R_2 = 2R_1$, we have $\frac{I_2}{I_1} = \left(\frac{2R_1}{R_1}\right)^4 = 2^4 = 16$.
Hence, $\frac{I_1}{I_2} = \frac{1}{16}$. Comparing with the given form $\frac{I_1}{I_2} = \frac{1}{x}$, we obtain $x = 16$.
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 : \(A_2 \rightleftharpoons 2A\)