Translational partition function
In statistical mechanics, the translational partition function, is that part of the partition function resulting from the movement (translation) of the center of mass. For a single atom or molecule in a low pressure gas, neglecting the interactions of molecules, the Canonical Ensemble can be approximated by:
Here, V is the volume of the container holding the molecule, Λ is the Thermal de Broglie wavelength, h is the Planck constant, m is the mass of a molecule, kB is the Boltzmann constant and T is the absolute temperature. This approximation is valid as long as Λ is much less than any dimension of the volume the atom or molecule is in. Since typical values of Λ are on the order of 10-100 pm, this is almost always an excellent approximation.
When considering a set of N non-interacting but identical atoms or molecules, when QT ≫ N , or equivalently when ρ Λ ≪ 1 where ρ is the density of particles, the total translational partition function can be written
The factor of N! arises from the restriction of allowed N particle states due to Quantum exchange symmetry . Most substances form liquids or solids at temperatures much higher than when when this approximation breaks down significantly.
- Donald A. McQuarrie, Statistical Mechanics, Harper \& Row, 1973
|This quantum mechanics-related article is a stub. You can help Wikipedia by expanding it.|