Born-Huggins-Meyer potential: Difference between revisions

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* <math> \sigma </math> is the  diameter (length), ''i.e.'' the value of <math>r</math> at which <math> \Phi_{12}(r)=0</math>
* <math> \sigma </math> is the  diameter (length), ''i.e.'' the value of <math>r</math> at which <math> \Phi_{12}(r)=0</math>


The first term is an exponentioal repulsion, followed by dipole-dipole and dipole-quadrupole dispersion terms. This potential is often augmented with a [[Coulomb's law | Coulombic interaction]].
The first term is an exponential repulsion, followed by dipole-dipole and dipole-quadrupole dispersion terms. This potential is often augmented with a [[Coulomb's law | Coulombic interaction]].


This potential is often used to study [[Realistic models | alkali halides]].
This potential is often used to study [[Realistic models | alkali halides]].

Latest revision as of 13:53, 18 February 2010

The Born-Huggins-Meyer potential (although looking at the authors/publications perhaps it would be more precisely known as the Born-Meyer-Huggins potential) [1] [2] [3] is given by [4]

where

  • is the intermolecular pair potential between two particles or sites
  • is the diameter (length), i.e. the value of at which

The first term is an exponential repulsion, followed by dipole-dipole and dipole-quadrupole dispersion terms. This potential is often augmented with a Coulombic interaction.

This potential is often used to study alkali halides.

References[edit]