Square well model

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The square well model is given by [1]

\[ \Phi_{12}\left( r \right) = \left\{ \begin{array}{ccc} \infty & ; & r < \sigma \\ - \epsilon & ; &\sigma \le r < \lambda \sigma \\ 0 & ; & r \ge \lambda \sigma \end{array} \right. \]

where \(\Phi_{12}(r)\) is the intermolecular pair potential, \(\epsilon\) is the well depth, \(r\) is the distance between site 1 and site 2 \(r := |\mathbf{r}_1 - \mathbf{r}_2|\), σ is the hard diameter and λ > 1. For an infinitesimally narrow well one has the sticky hard sphere model proposed by Baxter.

Contents

[edit] Equation of state

Main article: Equations of state for the square well model

[edit] Virial coefficients

Main article: Square well potential: virial coefficients

[edit] Liquid-vapour coexistence

[edit] Critical point

[edit] Direct correlation function

For the direct correlation function see:

[edit] References

  1. A. Rotenberg "Monte Carlo Equation of State for Hard Spheres in an Attractive Square Well", Journal of Chemical Physics 43 pp. 1198-1201 (1965)

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