The kinetic energy of other molecules does not involve the momentum of this particular molecule. Moreover, the potential energy of interaction between molecules depends only on their position coordinates, and, thus, certainly does not involve . Any internal rotational, vibrational, electronic, or nuclear degrees of freedom of the molecule also do not involve . Hence, the essential conditions of the equipartition theorem are satisfied (at least, in the classical approximation). Since Eq. (492) contains three independent quadratic terms, there are clearly three degrees of freedom associated with translation (one for each dimension of space), so the translational contribution to the molar heat capacity of gases is

Suppose that our gas is contained in a cubic enclosure of dimensions . According
to Schrödinger's equation, the quantized translational
energy levels of an individual molecule are given by

(494) |

The electronic degrees of freedom of gas molecules (*i.e.*, the possible
configurations of electrons orbiting the atomic nuclei) typically give rise
to absorption and emission in the
ultraviolet or visible regions of the spectrum. It follows from Tab. 3 that
electronic degrees of freedom are frozen out at room temperature. Similarly,
nuclear degrees of freedom (*i.e.*, the possible configurations of protons
and neutrons in the atomic nuclei) are frozen out because they are associated
with absorption and emission in the X-ray and -ray regions of the
electromagnetic spectrum. In fact, the only additional degrees of freedom
we need worry about for gases are rotational and vibrational degrees of freedom.
These typically give rise to absorption lines in the infrared region of the
spectrum.

The rotational kinetic energy of a molecule tumbling in space can be written

(495) |

(496) |

(497) |

Classically, the vibrational degrees of freedom of a molecule are studied by
standard normal mode analysis of the
molecular
structure. Each normal mode behaves like an
independent harmonic oscillator, and, therefore,
contributes to the molar specific heat of the gas [ from the
kinetic energy of vibration and from the potential energy of
vibration]. A molecule containing atoms has normal modes of vibration.
For instance, a diatomic molecule has just one normal mode (corresponding to
periodic stretching of the bond between the two atoms). Thus, the classical
contribution to the specific heat from vibrational degrees of freedom is

(498) |

So, do any of the rotational and vibrational degrees of freedom
actually make a contribution to the specific heats of gases at room temperature,
once quantum effects are taken into consideration? We can answer this
question by
examining just one piece of data. Figure 3 shows the
infrared absorption spectrum of Hydrogen Chloride. The absorption lines correspond
to simultaneous transitions between different vibrational and rotational energy
levels. Hence, this is usually called a *vibration-rotation spectrum*. The missing
line at about microns corresponds to a pure vibrational transition from the
ground-state to the first excited state (pure vibrational transitions are
*forbidden*: HCl molecules always have to simultaneously change their rotational energy level if they are to couple effectively to electromagnetic radiation).
The longer wavelength absorption lines correspond to vibrational transitions in
which there is a simultaneous decrease in the rotational energy level.
Likewise, the
shorter wavelength absorption lines correspond to vibrational transitions in which
there is a simultaneous increase in the rotational energy level. It is clear that
the rotational energy levels are more closely spaced than the vibrational energy
levels. The pure vibrational transition gives rise to absorption at
about microns, which corresponds to infrared radiation of frequency
hertz with an associated
radiation ``temperature'' of 4400 degrees kelvin. We
conclude that
the vibrational degrees of freedom of HCl, or any other small molecule,
are frozen out at room temperature. The rotational transitions split the
vibrational lines by about microns. This implies that pure rotational
transitions would be associated with infrared radiation of frequency
hertz and corresponding
radiation ``temperature'' 260 degrees kelvin. We
conclude that the rotational degrees of freedom of HCl, or any other small
molecule, are not frozen out at room temperature, and probably contribute the
classical to the molar specific heat. There is one proviso, however.
Linear molecules (like HCl) effectively only have two rotational degrees of
freedom (instead of the usual three), because of the very small moment
of inertia of such molecules along the line of centres of the atoms.

We are now in a position to make some predictions regarding the specific heats
of various gases. Monatomic molecules only possess three translational degrees
of freedom, so monatomic gases should have a molar heat capacity
joules/degree/mole. The ratio of specific heats
should be . It can be seen from Tab. 2 that both of
these predictions are borne out pretty well for Helium and Argon.
Diatomic molecules possess three translational degrees of freedom and
two rotational degrees of freedom (all other degrees of freedom are frozen out
at room temperature). Thus, diatomic gases should have a molar heat capacity
joules/degree/mole. The ratio of specific heats should be
. It can be seen from Tab. 2 that these are pretty accurate
predictions for Nitrogen and Oxygen. The freezing out of vibrational
degrees of freedom becomes gradually less effective as molecules become heavier
and more complex. This is partly because such molecules are generally less
stable, so the force constant is reduced, and partly
because the molecular mass
is increased. Both these effect reduce the frequency of vibration of the
molecular normal
modes [see Eq. (472)], and, hence, the spacing between vibrational energy levels
[see Eq. (471)]. This accounts for the obviously non-classical [*i.e.*, not
a multiple of ] specific heats of Carbon Dioxide and Ethane in
Tab. 2.
In both molecules, vibrational degrees of freedom contribute to the molar specific
heat (but not the full because the temperature is not high enough).

Figure 4 shows the variation of the molar heat capacity at constant volume (in units of ) of gaseous hydrogen with temperature. The expected contribution from the translational degrees of freedom is (there are three translational degrees of freedom per molecule). The expected contribution at high temperatures from the rotational degrees of freedom is (there are effectively two rotational degrees of freedom per molecule). Finally, the expected contribution at high temperatures from the vibrational degrees of freedom is (there is one vibrational degree of freedom per molecule). It can be seen that as the temperature rises the rotational, and then the vibrational, degrees of freedom eventually make their full classical contributions to the heat capacity.