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:
$35 \, K_B T$

An infinitely long straight wire carrying current $I$ is bent in a planar shape as shown in the diagram. The radius of the circular part is $r$. The magnetic field at the centre $O$ of the circular loop is :




Consider the following reaction sequence.

Foot of perpendicular from origin on a line passing through $(1, 1, 1)$ having direction ratios $\langle 2, 3, 4 \rangle$, is: