Yes fair enough. That just goes to show how hard it is for a chemist to set aside QM thinking!
In fact, the specific heat of gases is one of the classic results of Stat TD - but based, as you rightly remind me, on QM assumptions about energy level spacing in the various degrees of freedom and how they are populated: ε >> kT vs. ε << kT .
In fact, the *wrong* prediction of specific heats for larger molecules was one of the first hints of quantization. Classical descriptions worked reasonably well for monatomic and diatomic gases, but got increasingly bad for gases like methane. In a classical setting, methane would have a very large number of degrees of freedom, each with average energy kT. This would make the specific heat much smaller than what was observed.
The resolution? Energy levels with E>>kT are not populated at all, so the average energy is NOT kT in the quantum version.
Moreover, the Maxwell distribution exp(-kT/E) is replaced by either the Fermi or the Bose distribution (depending on total spins). This is more relevant for solid state physics, though, as opposed to gas state.