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:
$35 \, K_B T$
For an ideal gas, a cyclic process ABCA as shown in the P–T diagram. When represented in P–V plot, it would be 

The heat generated in 1 minute between points A and B in the given circuit, when a battery of 9 V with internal resistance of 1 \(\Omega\) is connected across these points is ______ J. 
The given circuit works as: 
Let the lines $L_1 : \vec r = \hat i + 2\hat j + 3\hat k + \lambda(2\hat i + 3\hat j + 4\hat k)$, $\lambda \in \mathbb{R}$ and $L_2 : \vec r = (4\hat i + \hat j) + \mu(5\hat i + + 2\hat j + \hat k)$, $\mu \in \mathbb{R}$ intersect at the point $R$. Let $P$ and $Q$ be the points lying on lines $L_1$ and $L_2$, respectively, such that $|PR|=\sqrt{29}$ and $|PQ|=\sqrt{\frac{47}{3}}$. If the point $P$ lies in the first octant, then $27(QR)^2$ is equal to}