Stockmayer potential: Difference between revisions
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* <math>\theta_1,\theta_2 </math> is the inclination of the two dipole axes with respect to the intermolecular axis. | * <math>\theta_1,\theta_2 </math> is the inclination of the two dipole axes with respect to the intermolecular axis. | ||
* <math>\phi</math> is the azimuth angle between the two dipole moments | * <math>\phi</math> is the azimuth angle between the two dipole moments | ||
If one defines | If one defines a reduced dipole moment, <math>\mu^*</math>, such that: | ||
:<math>\mu^* := \sqrt{\frac{\mu^2}{4\pi\epsilon_0\epsilon \sigma^3}}</math> | :<math>\mu^* := \sqrt{\frac{\mu^2}{4\pi\epsilon_0\epsilon \sigma^3}}</math> |
Revision as of 12:42, 3 December 2010
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 r;
- is the diameter (length), i.e. the value of at ;
- : well depth (energy)
- is the permittivity of the vacuum
- is the dipole moment
- is 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]:
References
Related reading
- M. E. van Leeuwen "Derivation of Stockmayer potential parameters for polar fluids", Fluid Phase Equilibria 99 pp. 1-18 (1994)
- Reinhard Hentschke, Jörg Bartke, and Florian Pesth "Equilibrium polymerization and gas-liquid critical behavior in the Stockmayer fluid", Physical Review E 75 011506 (2007)