Continuous shouldered well model
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The continuous shouldered well model is given by (
\[\Phi_{12}(r) = \frac{U_R}{1 + \exp [\Delta(r-R_R)/a]} -U_A \exp \left[ -\frac{(r-R_A)^2}{2\delta_A^2} \right] + \left(\frac{a}{r}\right)^{24}\]
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
- ↑ 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)
Related reading
- Alan Barros de Oliveira, Giancarlo Franzese, Paulo A. Netz, and Marcia C. Barbosa "Waterlike hierarchy of anomalies in a continuous spherical shouldered potential", Journal ofChemical Physics 128 064901 (2008)
- Pol Vilaseca and Giancarlo Franzese "Softness dependence of the anomalies for the continuous shouldered well potential", Journal of Chemical Physics 133 084507 (2010)