For a non-rigid diatomic molecule, the degrees of freedom \( f \) are given by:
\[f = 5 + 2(3N - 5)\]
Since \( N = 2 \) (for diatomic molecules):
\[f = 5 + 2(3 \times 2 - 5) = 7\]
The energy of one molecule is:
\[\text{Energy} = \frac{f}{2} k_B T = \frac{7}{2} k_B T\]
For 10 molecules, the total energy is:
\[10 \times \frac{7}{2} k_B T = 35 k_B T\]
To determine the energy of 10 non-rigid diatomic molecules at temperature \( T \), we need to consider the degrees of freedom available to a non-rigid diatomic molecule and apply the principles of statistical mechanics.
Diatomic molecules, unlike monatomic molecules, have additional degrees of freedom due to their rotational and vibrational motions. In the case of non-rigid diatomic molecules:
Total degrees of freedom for a non-rigid diatomic molecule = 3 (translational) + 2 (rotational) + 2 (vibrational) = 7.
According to the equipartition theorem, each degree of freedom contributes \(\frac{1}{2} k_B T\) to the energy at thermal equilibrium, where \( k_B \) is the Boltzmann constant.
Hence, the energy per molecule is:
\(E = \frac{7}{2} k_B T\)
For 10 molecules, the total energy will be:
\(E_{\text{total}} = 10 \times \frac{7}{2} k_B T = 35 k_B T\)
Thus, the total energy for 10 non-rigid diatomic molecules at temperature \( T \) is:
\(35 \, K_B T\)
Therefore, the correct answer is:
$35 \, K_B T$
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 : \(A_2 \rightleftharpoons 2A\)