Continuous shouldered well model

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The continuous shouldered well model is given by ([1] Eq. 1):

\[\Phi_{12}(r) = \frac{U_R}{1 + \exp [\Delta(r-R_R)/a]} -U_A \exp \left[ -\frac{(r-R_A)^2}{2\delta_A^2} \right] + \left(\frac{a}{r}\right)^{24}\]

where \(\Phi_{12}\) is the intermolecular pair potential, \(U_R\) is the energy of the repulsive shoulder, \(U_A\) is the energy of the attractive well, \(a\) is the diameter of the particles, and \(r := |\mathbf{r}_1 - \mathbf{r}_2|\).

[edit] References

  1. Giancarlo Franzese "Differences between discontinuous and continuous soft-core attractive potentials: The appearance of density anomaly", Journal of Molecular Liquids 136 pp. 267-273 (2007)

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