Kern and Frenkel patchy model: Difference between revisions
Carl McBride (talk | contribs) m (Added Hard ellipsoid model variant) |
No edit summary |
||
Line 21: | Line 21: | ||
f_{ij} \left(\hat{ {\mathbf r}}_{ij}; \tilde{ {\mathbf \Omega}}_i, \tilde{ {\mathbf \Omega}}_j \right) = | f_{ij} \left(\hat{ {\mathbf r}}_{ij}; \tilde{ {\mathbf \Omega}}_i, \tilde{ {\mathbf \Omega}}_j \right) = | ||
\left\{ \begin{array}{clc} | \left\{ \begin{array}{clc} | ||
1 & \mathrm{if} & \left\{ \begin{array}{ccc} & (\hat{e}_\alpha\cdot\hat{r}_{ij} \ | 1 & \mathrm{if} & \left\{ \begin{array}{ccc} & (\hat{e}_\alpha\cdot\hat{r}_{ij} \geq \cos \delta) & \mathrm{for~some~patch~\alpha~on~}i \\ | ||
\mathrm{and} & (\hat{e}_\beta\cdot\hat{r}_{ji} \ | \mathrm{and} & (\hat{e}_\beta\cdot\hat{r}_{ji} \geq \cos \delta) & \mathrm{for~some~patch~\beta~on~}j \end{array} \right. \\ | ||
0 & \mathrm{otherwise} & \end{array} \right. | 0 & \mathrm{otherwise} & \end{array} \right. | ||
</math> | </math> |
Revision as of 22:03, 25 May 2021
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)
where the radial component is given by the square well model (Eq. 2)
and the orientational component is given by (Eq. 3)
where is the solid angle of a patch () whose axis is (see Fig. 1 of Ref. 1), forming a conical segment.
Two patches
The "two-patch" Kern and Frenkel model has been extensively studied by Sciortino and co-workers [2][3][4].
Four patches
- Main article: Anisotropic particles with tetrahedral symmetry
Single-bond-per-patch-condition
If the two parameters and fullfil the condition
then the patch cannot be involved in more than one bond. Enforcing this condition makes it possible to compare the simulations results with Wertheim theory [2][4]
Hard ellipsoid model
The hard ellipsoid model has also been used as the 'nucleus' of the Kern and Frenkel patchy model [5].
References
- ↑ Norbert Kern and Daan Frenkel "Fluid–fluid coexistence in colloidal systems with short-ranged strongly directional attraction", Journal of Chemical Physics 118, 9882 (2003)
- ↑ 2.0 2.1 F. Sciortino, E. Bianchi, J. Douglas and P. Tartaglia "Self-assembly of patchy particles into polymer chains: A parameter-free comparison between Wertheim theory and Monte Carlo simulation", Journal of Chemical Physics 126 194903 (2007)
- ↑ Achille Giacometti, Fred Lado, Julio Largo, Giorgio Pastore, and Francesco Sciortino "Effects of patch size and number within a simple model of patchy colloids", Journal of Chemical Physics 132, 174110 (2010)
- ↑ 4.0 4.1 José Maria Tavares, Lorenzo Rovigatti, and Francesco Sciortino "Quantitative description of the self-assembly of patchy particles into chains and rings", Journal of Chemical Physics 137 044901 (2012)
- ↑ T. N. Carpency, J. D. Gunton and J. M. Rickman "Phase behavior of patchy spheroidal fluids", Journal of Chemical Physics 145 214904 (2016)
- Related reading
- 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)
- 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)
- Z. Preisler, T. Vissers, F. Smallenburg and F. Sciortino "Crystals of Janus colloids at various interaction ranges", Journal of Chemical Physics 145 064513 (2016)