1-dimensional hard rods are basically hard spheres confined to 1 dimension (not to be confused with 3-dimensional hard rods). The model is given by the intermolecular pair potential:
where is the position of the center of the k-th rod, along with an external potential; the whole length of the rod must be inside the range:
Canonical Ensemble: Configuration Integral
The statistical mechanics of this system can be solved exactly (see Ref. 1).
Consider a system of length defined in the range . The aim is to compute the partition function of a system of hard rods of length .
Consider that the particles are ordered according to their label: ;
taking into account the pair potential we can write the canonical partition function
(configuration integral)
of a system of particles as:
Variable change: ; we get:
Therefore:
Thermodynamics
Helmholtz energy function
In the thermodynamic limit (i.e. with , remaining finite):
Equation of state
Using the thermodynamic relations, the pressure (linear tension in this case) can
be written as:
where ; is the fraction of volume (i.e. length) occupied by the rods.
References
- Lewi Tonks "The Complete Equation of State of One, Two and Three-Dimensional Gases of Hard Elastic Spheres", Physical Review 50 pp. 955- (1936)
- L. van Hove "Quelques Propriétés Générales De L'intégrale De Configuration D'un Système De Particules Avec Interaction", Physica, 15 pp. 951-961 (1949)
- L. van Hove, "Sur L'intégrale de Configuration Pour Les Systèmes De Particules À Une Dimension", Physica, 16 pp. 137-143 (1950)