Stockmayer potential: Difference between revisions

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The '''Stockmayer potential''' consists of the [[Lennard-Jones model]] with an embedded point dipole. Thus the Stockmayer potential becomes:
The '''Stockmayer potential''' consists of the [[Lennard-Jones model]] with an embedded point [[Dipole moment |dipole]]. Thus the Stockmayer potential becomes (Eq. 1 <ref>[http://dx.doi.org/10.1063/1.1750922 W. H. Stockmayer "Second Virial Coefficients of Polar Gases", Journal of Chemical Physics '''9''' pp. 398-402 (1941)]</ref>):


:<math> \Phi(r, \theta_1, \theta_2, \phi) = 4 \epsilon \left[ \left(\frac{\sigma}{r} \right)^{12}-  \left( \frac{\sigma}{r}\right)^6 \right] - \frac{\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) </math>
:<math> \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) </math>


where:
where:
* <math> \Phi(r) </math> is the [[intermolecular pair potential]] between two particles at a distance r;
* <math>r := |\mathbf{r}_1 - \mathbf{r}_2|</math>
* <math> \sigma </math> is the  diameter (length), i.e. the value of <math>r</math> at <math> \Phi(r)=0</math> ;
* <math> \Phi(r) </math> is the [[intermolecular pair potential]] between two particles at a distance <math>r</math>
* <math> \epsilon </math> : well depth (energy)
* <math> \sigma </math> is the  diameter (length), i.e. the value of <math>r</math> at <math> \Phi(r)=0</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,\theta_2 </math> is the inclination of the two dipole axes with respect to the intermolecular axis.
* <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 the reduced dipole moment, <math>\mu^*</math>  
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>
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For this reason the potential is sometimes known as the Stockmayer 12-6-3 potential.
For this reason the potential is sometimes known as the Stockmayer 12-6-3 potential.
==Critical properties==
In the range <math>0 \leq \mu^* \leq 2.45</math> <ref>[http://dx.doi.org/10.1080/00268979400100294 M.E. Van Leeuwen "Deviation from corresponding-states behaviour for polar fluids", Molecular Physics '''82''' pp. 383-392 (1994)]</ref>:
:<math>T_c^* = 1.313 + 0.2999\mu^{*2} -0.2837 \ln(\mu^{*2} +1)</math>
:<math>\rho_c^* = 0.3009 - 0.00785\mu^{*2} - 0.00198\mu^{*4}</math>
:<math>P_c^* = 0.127 + 0.0023\mu^{*2}</math>
==Bridge function==
A [[bridge function]] for use in [[integral equations]] has been calculated by Puibasset and Belloni <ref>[http://dx.doi.org/10.1063/1.4703899 Joël Puibasset and Luc Belloni "Bridge function for the dipolar fluid from simulation", Journal of Chemical Physics '''136''' 154503 (2012)]</ref>.
==References==
<references/>
'''Related reading'''
*[http://www.nrcresearchpress.com/doi/abs/10.1139/v77-418 Frank M. Mourits, Frans H. A. Rummens "A critical evaluation of Lennard–Jones and Stockmayer potential parameters and of some correlation methods", Canadian Journal of Chemistry '''55''' pp. 3007-3020 (1977)]
*[http://dx.doi.org/10.1016/0378-3812(94)80018-9 M. E. van Leeuwen "Derivation of Stockmayer potential parameters for polar fluids", Fluid Phase Equilibria '''99''' pp. 1-18 (1994)]
*[http://dx.doi.org/10.1016/j.fluid.2007.02.009 Osvaldo H. Scalise "On the phase equilibrium Stockmayer fluids", Fluid Phase Equilibria '''253''' pp. 171–175 (2007)]
*[http://dx.doi.org/10.1103/PhysRevE.75.011506  Reinhard Hentschke, Jörg Bartke, and Florian Pesth "Equilibrium polymerization and gas-liquid critical behavior in the Stockmayer fluid", Physical Review E '''75''' 011506 (2007)]
*[http://dx.doi.org/10.1063/1.4821455  Jun Wang , Pankaj A. Apte , James R. Morris  and Xiao Cheng Zeng "Freezing point and solid-liquid interfacial free energy of Stockmayer dipolar fluids: A molecular dynamics simulation study", Journal of Chemical Physics '''139''' 114705 (2013)]


==References==
{{numeric}}
#[http://dx.doi.org/10.1080/00268979400100294 M. E. Van Leeuwe "Deviation from corresponding-states behaviour for polar fluids", Molecular Physics '''82''' pp. 383-392 (1994)]
[[category: models]]
[[category: models]]

Latest revision as of 16:39, 6 November 2013

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[edit]

In the range [2]:

Bridge function[edit]

A bridge function for use in integral equations has been calculated by Puibasset and Belloni [3].

References[edit]

Related reading

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