Stockmayer potential: Difference between revisions
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where: | where: | ||
* <math>r := |\mathbf{r}_1 - \mathbf{r}_2|</math> | * <math>r := |\mathbf{r}_1 - \mathbf{r}_2|</math> | ||
* <math> \Phi(r) </math> is the [[intermolecular pair potential]] between two particles at a distance r | * <math> \Phi(r) </math> is the [[intermolecular pair potential]] between two particles at a distance <math>r</math> | ||
* <math> \sigma </math> is the diameter (length), i.e. the value of <math>r</math> at <math> \Phi(r)=0</math> | * <math> \sigma </math> is the diameter (length), i.e. the value of <math>r</math> at <math> \Phi(r)=0</math> | ||
* <math> \epsilon </math> | * <math> \epsilon </math> represents the well depth (energy) | ||
* <math> \epsilon_0 </math> is the permittivity of the vacuum | * <math> \epsilon_0 </math> is the permittivity of the vacuum | ||
* <math>\mu</math> is the dipole moment | * <math>\mu</math> is the dipole moment | ||
* <math>\theta_1 | * <math>\theta_1</math> and <math>\theta_2 </math> are the angles associated with 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 a reduced dipole moment, <math>\mu^*</math>, such that: | If one defines a reduced dipole moment, <math>\mu^*</math>, such that: |
Revision as of 12:44, 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
- 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]:
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)