Square shoulder + square well model: Difference between revisions

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The '''Square shoulder + square well''' model consists, as its name suggests, of a combination of the [[square shoulder model]] and the [[square well model]]. The model is given by
:<math>
\Phi_{12}\left( r \right) =
\left\{ \begin{array}{ccc}
\infty & ; & r < \sigma \\
\epsilon_1 & ; &\sigma \le r < \lambda_1 \sigma \\
- \epsilon_2 & ; &\lambda_1\sigma \le r < \lambda_2 \sigma \\
0        & ; & r \ge \lambda_2 \sigma \end{array} \right.
</math>
where <math>\Phi_{12}(r)</math> is the [[intermolecular pair potential]], <math>\epsilon_1</math> and <math>\epsilon_2</math> are the well ''depths'', <math>r</math> is the distance between site 1 and site 2  where <math>r := |\mathbf{r}_1 - \mathbf{r}_2|</math>, &sigma; is the hard core diameter
and <math>\lambda_1,\lambda_2>1</math>
==Critical points==
See Ref. 2.
==References==
==References==
#[http://dx.doi.org/10.1088/0953-8984/11/50/308 Andreas Lang, Gerhard Kahl, Christos N Likos, Hartmut Löwen and Martin Watzlawek "Structure and thermodynamics of square-well and square-shoulder fluids", Journal of Physics: Condensed Matter '''11''' pp. 10143-10161  (1999)]
#[http://dx.doi.org/10.1088/0953-8984/11/50/308 Andreas Lang, Gerhard Kahl, Christos N Likos, Hartmut Löwen and Martin Watzlawek "Structure and thermodynamics of square-well and square-shoulder fluids", Journal of Physics: Condensed Matter '''11''' pp. 10143-10161  (1999)]
#[http://dx.doi.org/10.1063/1.2970884 W. Rzysko, O. Pizio, A. Patrykiejew, and S. Sokolowski "Phase diagram of a square-shoulder, square-well fluid revisited", Journal of Chemical Physics '''129''' 124502 (2008)]
[[Category: Models]]
[[Category: Models]]
[[category: Polyamorphic systems]]
[[category: Polyamorphic systems]]

Revision as of 09:29, 25 September 2008

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The Square shoulder + square well model consists, as its name suggests, of a combination of the square shoulder model and the square well model. The model is given by

Φ12(r)={∞;r<σϵ1;σ≤r<λ1σ−ϵ2;λ1σ≤r<λ2σ0;r≥λ2σ

where Φ12(r) is the intermolecular pair potential, ϵ1 and ϵ2 are the well depths, r is the distance between site 1 and site 2 where r:=|r1−r2|, σ is the hard core diameter and λ1,λ2>1

Critical points

See Ref. 2.

References

  1. Andreas Lang, Gerhard Kahl, Christos N Likos, Hartmut Löwen and Martin Watzlawek "Structure and thermodynamics of square-well and square-shoulder fluids", Journal of Physics: Condensed Matter 11 pp. 10143-10161 (1999)
  2. W. Rzysko, O. Pizio, A. Patrykiejew, and S. Sokolowski "Phase diagram of a square-shoulder, square-well fluid revisited", Journal of Chemical Physics 129 124502 (2008)