Stockmayer potential
The Stockmayer potential consists of the Lennard-Jones model with an embedded point dipole. Thus the Stockmayer potential becomes (Eq. 1 [1]):
where:
- is the intermolecular pair potential between two particles at a distance
- is the diameter (length), i.e. the value of at
- represents the well depth (energy)
- is the permittivity of the vacuum
- is the dipole moment
- and are the angles associated with the inclination of the two dipole axes with respect to the intermolecular axis.
- is the azimuth angle between the two dipole moments
If one defines a reduced dipole moment, , such that:
one can rewrite the expression as
For this reason the potential is sometimes known as the Stockmayer 12-6-3 potential.
Critical properties
In the range [2]:
Bridge function
A bridge function for use in integral equations has been calculated by Puibasset and Belloni [3].
References
- ↑ W. H. Stockmayer "Second Virial Coefficients of Polar Gases", Journal of Chemical Physics 9 pp. 398-402 (1941)
- ↑ M.E. Van Leeuwen "Deviation from corresponding-states behaviour for polar fluids", Molecular Physics 82 pp. 383-392 (1994)
- ↑ Joël Puibasset and Luc Belloni "Bridge function for the dipolar fluid from simulation", Journal of Chemical Physics 136 154503 (2012)
Related reading
- M. E. van Leeuwen "Derivation of Stockmayer potential parameters for polar fluids", Fluid Phase Equilibria 99 pp. 1-18 (1994)
- Osvaldo H. Scalise "On the phase equilibrium Stockmayer fluids", Fluid Phase Equilibria 253 pp. 171–175 (2007)
- Reinhard Hentschke, Jörg Bartke, and Florian Pesth "Equilibrium polymerization and gas-liquid critical behavior in the Stockmayer fluid", Physical Review E 75 011506 (2007)