N-6 Lennard-Jones potential: Difference between revisions

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m ("explained" the 12 subscript for Phi)
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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_{12}(r) </math> is the [[intermolecular pair potential]] between two particles or ''sites''
* <math> \Phi_{12}(r) </math> is the [[intermolecular pair potential]] between two particles, "1" and "2".
* <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>
* <math> \epsilon </math> is the well depth (energy)
* <math> \epsilon </math> is the well depth (energy)

Revision as of 11:30, 13 October 2011

The n-6 Lennard-Jones potential is a variant the more well known Lennard-Jones model (or from a different point of view, a particular case of the Mie potential).. The potential is given by [1]:

where

  • is the intermolecular pair potential between two particles, "1" and "2".
  • is the diameter (length), i.e. the value of at which
  • is the well depth (energy)

Melting point

An approximate method to locate the melting point is given in [2].

References

Related reading