Continuous shouldered well model: Difference between revisions

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{{stub-general}}
The '''continuous shouldered well model''' ('''CSW''') is given by (<ref>[http://dx.doi.org/10.1016/j.molliq.2007.08.021  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)]</ref> Eq. 1):
The '''continuous shouldered well model''' is given by (Ref. 1 Eq. 1):


:<math>\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}</math>
:<math>\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}</math>
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where <math>\Phi_{12}</math> is the [[intermolecular pair potential]], <math>U_R</math> is the energy of the repulsive shoulder, <math>U_A</math> is the energy of the attractive well, <math>a</math> is the diameter of the particles, and  <math>r := |\mathbf{r}_1 - \mathbf{r}_2|</math>.
where <math>\Phi_{12}</math> is the [[intermolecular pair potential]], <math>U_R</math> is the energy of the repulsive shoulder, <math>U_A</math> is the energy of the attractive well, <math>a</math> is the diameter of the particles, and  <math>r := |\mathbf{r}_1 - \mathbf{r}_2|</math>.
==References==  
==References==  
#[http://dx.doi.org/10.1016/j.molliq.2007.08.021 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)]
<references/>
#[http://dx.doi.org/10.1063/1.2830706 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)]
'''Related reading'''
*[http://dx.doi.org/10.1063/1.2830706 Alan Barros de Oliveira, Giancarlo Franzese, Paulo A. Netz, and Marcia C. Barbosa "Waterlike hierarchy of anomalies in a continuous spherical shouldered potential", Journal of Chemical Physics '''128''' 064901 (2008)]
*[http://dx.doi.org/10.1063/1.3463424  Pol Vilaseca and Giancarlo Franzese "Softness dependence of the anomalies for the continuous shouldered well potential", Journal of Chemical Physics '''133''' 084507 (2010)]
*[http://dx.doi.org/10.1063/1.4809744  Matej Huš , Matja Zalar  and Tomaz Urbic "Correctness of certain integral equation theories for core-softened fluids", Journal of Chemical Physics '''138''' 224508 (2013)]
*[http://dx.doi.org/10.1063/1.4909550  L. A. Cervantes, G. Jaime-Muñoz, A. L. Benavides, J. Torres-Arenas, and F. Sastre "Discrete perturbation theory for continuous soft-core potential fluids", Journal of Chemical Physics '''142''' 114501 (2015)]
*[http://dx.doi.org/10.1016/j.molliq.2016.10.030 Miha Lukšič, Barbara Hribar-Lee, and Orest Pizio "Phase behaviour of a continuous shouldered well model fluid. A grand canonical Monte Carlo study", Journal of Molecular Liquids '''228''' pp. 4-10 (2017)]
 
[[Category: Models]]
[[Category: Models]]

Latest revision as of 13:48, 3 February 2017

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

where is the intermolecular pair potential, is the energy of the repulsive shoulder, is the energy of the attractive well, is the diameter of the particles, and .

References[edit]

Related reading