Kern and Frenkel patchy model: Difference between revisions

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*[http://dx.doi.org/10.1063/1.3689308 Christoph Gögelein, Flavio Romano, Francesco Sciortino, and Achille Giacometti "Fluid-fluid and fluid-solid transitions in the Kern-Frenkel model from Barker-Henderson thermodynamic perturbation theory", Journal of Chemical Physics '''136''' 094512 (2012)]
*[http://dx.doi.org/10.1063/1.3689308 Christoph Gögelein, Flavio Romano, Francesco Sciortino, and Achille Giacometti "Fluid-fluid and fluid-solid transitions in the Kern-Frenkel model from Barker-Henderson thermodynamic perturbation theory", Journal of Chemical Physics '''136''' 094512 (2012)]
*[http://dx.doi.org/10.1063/1.4722477 Emanuela Bianchi, Günther Doppelbauer, Laura Filion, Marjolein Dijkstra, and Gerhard Kahl "Predicting patchy particle crystals: Variable box shape simulations and evolutionary algorithms", Journal of Chemical Physics '''136''' 214102 (2012)]
[[category: models]]
[[category: models]]

Revision as of 14:58, 7 June 2012

The Kern and Frenkel [1] patchy model is an amalgamation of the hard sphere model with attractive square well patches (HSSW). The potential has an angular aspect, given by (Eq. 1)


Φij(rij;Ω~i,Ω~j)=ΦijHSSW(rij)⋅f(Ω~i,Ω~j)


where the radial component is given by the square well model (Eq. 2)

ΦijHSSW(rij)={∞;r<σ−ϵ;σ≤r<λσ0;r≥λσ

and the orientational component is given by (Eq. 3)

fij(r^ij;Ω~i,Ω~j)={1if{(e^α⋅r^ij≤cosδ)forsomepatchαoniand(e^β⋅r^ji≤cosδ)forsomepatchβonj0otherwise

where δ is the solid angle of a patch (α,β,...) whose axis is e^ (see Fig. 1 of Ref. 1), forming a conical segment.

Two patches

The "two-patch" Kern and Frenkel model has been extensively studied by Giacometti et al. [2].

Four patches

Main article: Anisotropic particles with tetrahedral symmetry

References

Related reading