The translational, vibrational, and rotational molecular partition functions for a system containing ideal diatomic gas molecules in the canonical ensemble (N, V, T) are written as, $q_{trans}$, $q_{vib}$, and $q_{rot}$, respectively. The option that correctly defines their thermodynamic variable(s) dependency is
The question asks for the thermodynamic variables upon which the translational ($q_{trans}$), vibrational ($q_{vib}$), and rotational ($q_{rot}$) molecular partition functions depend for ideal diatomic gas molecules in the canonical ensemble (N, V, T).
The translational partition function depends on the available volume ($V$) and temperature ($T$). It describes the motion of the center of mass of the molecule. Its dependence is given by $q_{trans} \propto V T^{3/2}$. Therefore, $q_{trans}$ depends on both T and V.
The vibrational partition function depends on the vibrational frequency of the molecule (a molecular property) and the temperature ($T$). For ideal gases, vibrational energy levels are generally considered independent of the volume ($V$). Thus, $q_{vib}$ depends only on T.
The rotational partition function depends on the rotational constants (related to the moment of inertia, a molecular property) and the temperature ($T$). For ideal diatomic gases, rotational energy levels are also independent of the volume ($V$). Hence, $q_{rot}$ depends only on T.
Based on the analysis:
This matches the dependencies stated in Option B.
If $q_t$ and $Q_{t,m}$ are the molecular and molar translational partition functions of $X_2$, respectively, then $ln(Q_{t,m})$ =
(N is the Avogadro number)