The moment of inertia of a solid sphere about its diameter is given by the formula:
\( I_{\text{sphere}} = \frac{2}{5}mr^2 \)
where: - \( m \) is the mass of the sphere, - \( r \) is the radius of the sphere.
The parallel axis theorem states that the moment of inertia of a body about an axis parallel to and a distance \( d \) away from an axis through its center of mass is given by:
\( I = I_{\text{cm}} + md^2 \)
where: - \( I_{\text{cm}} \) is the moment of inertia about the center of mass axis, - \( d \) is the distance from the center of mass to the new axis.
The distance between the center of a sphere and the midpoint of the rod is:
\( d = \frac{40}{2} \, \text{cm} = 20 \, \text{cm} = 0.2 \, \text{m} \)
The radius of each sphere is \( r = 10 \, \text{cm} = 0.1 \, \text{m} \). Using the parallel axis theorem, the moment of inertia of one sphere about the midpoint of the rod is:
\( I_{\text{one}} = \frac{2}{5}mr^2 + md^2 \)
Substitute the values into the equation:
\( I_{\text{one}} = \frac{2}{5}(2)(0.1)^2 + (2)(0.2)^2 = 0.008 + 0.08 = 0.088 \, \text{kg-m}^2 \)
Since there are two identical spheres, the total moment of inertia of the system is:
\( I_{\text{sys}} = 2 \times I_{\text{one}} = 2 \times 0.088 = 0.176 \, \text{kg-m}^2 = 176 \times 10^{-3} \, \text{kg-m}^2 \)
The moment of inertia of the system is \( \mathbf{176 \times 10^{-3} \, \text{kg-m}^2} \).
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 : \(A_2 \rightleftharpoons 2A\)