The Stockmayer potential consists of the Lennard-Jones model with an embedded point dipole. Thus the Stockmayer potential becomes (Eq. 1 [1]):
![{\displaystyle \Phi _{12}(r,\theta _{1},\theta _{2},\phi )=4\epsilon \left[\left({\frac {\sigma }{r}}\right)^{12}-\left({\frac {\sigma }{r}}\right)^{6}\right]-{\frac {\mu _{1}\mu _{2}}{4\pi \epsilon _{0}r^{3}}}\left(2\cos \theta _{1}\cos \theta _{2}-\sin \theta _{1}\sin \theta _{2}\cos \phi \right)}](https://wikimedia.org/api/rest_v1/media/math/render/svg/564c2d6f35bed1a1be79385c43a1637bc2c917fb) 
where:
 
 is the intermolecular pair potential between two particles at a distance is the intermolecular pair potential between two particles at a distance 
 is the  diameter (length), i.e. the value of is the  diameter (length), i.e. the value of at at 
 represents the well depth (energy) represents the well depth (energy)
 is the permittivity of the vacuum is the permittivity of the vacuum
 is the dipole moment is the dipole moment
 and and are the angles associated with the inclination of the two dipole axes with respect to the intermolecular axis. 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 is the azimuth angle between the two dipole moments
If one defines a reduced dipole moment,  , such that:
, such that: 
 
one can rewrite the expression as 
![{\displaystyle \Phi (r,\theta _{1},\theta _{2},\phi )=\epsilon \left\{4\left[\left({\frac {\sigma }{r}}\right)^{12}-\left({\frac {\sigma }{r}}\right)^{6}\right]-\mu ^{*2}\left(2\cos \theta _{1}\cos \theta _{2}-\sin \theta _{1}\sin \theta _{2}\cos \phi \right)\left({\frac {\sigma }{r}}\right)^{3}\right\}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/936327d17871c7d4d826370da2a5aea503b43ebf) 
For this reason the potential is sometimes known as the Stockmayer 12-6-3 potential.
Critical properties
In the range  [2]:
 [2]:
 
 
 
References
Related reading
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