Hard core Yukawa potential: Difference between revisions
mNo edit summary |
Carl McBride (talk | contribs) m (Replaced mention of a model with a See also section) |
||
(20 intermediate revisions by 3 users not shown) | |||
Line 1: | Line 1: | ||
The '''hard core Yukawa''' potential <ref>[http://dx.doi.org/10.1016/0378-4371(89)90108-8 J. S. Rowlinson "The Yukawa potential", Physica A: Statistical Mechanics and its Applications '''156''' pp. 15-34 (1989)]</ref> | |||
has two forms, the attractive Yukawa potential: | |||
:<math> | :<math> | ||
\ | \Phi_{12}\left( r \right) = | ||
\left\{ \begin{array}{lll} | \left\{ \begin{array}{lll} | ||
\infty & ; & r < \sigma \\ | \infty & ; & r < \sigma \\ | ||
Line 9: | Line 10: | ||
</math> | </math> | ||
where <math> \Phi\left( r \right) </math> is the [[intermolecular pair potential]], <math> r </math> is the distance, | and the repulsive form | ||
:<math> | |||
\Phi_{12}\left( r \right) = | |||
\left\{ \begin{array}{lll} | |||
\infty & ; & r < \sigma \\ | |||
\left( \frac{ \epsilon \sigma }{r}\right) \exp \left[- \kappa \left( \frac{r}{\sigma} - 1 \right) \right] & ; & r \ge \sigma | |||
\end{array} \right. | |||
</math> | |||
where <math> \Phi\left( r \right) </math> is the [[intermolecular pair potential]], <math>r := |\mathbf{r}_1 - \mathbf{r}_2|</math> is the distance between site 1 and site 2, | |||
<math> \sigma </math> is the hard diameter, <math> \epsilon </math> is the energy well depth (<math> \epsilon > 0 </math>), and | <math> \sigma </math> is the hard diameter, <math> \epsilon </math> is the energy well depth (<math> \epsilon > 0 </math>), and | ||
<math> \kappa </math> is a parameter that controls the interaction range (<math> \kappa > 0 </math>). | <math> \kappa </math> is a parameter that controls the interaction range (<math> \kappa > 0 </math>). | ||
The repulsive form has been used to study charge-stabilised [[Colloids |colloid-colloid]] interactions. | |||
==Critical point== | |||
For the attractive form of the potential, from a study of the [[law of corresponding states]], one has (Eq. 3 in <ref>[http://dx.doi.org/10.1063/1.2883694 Pedro Orea and Yurko Duda "On the corresponding states law of the Yukawa fluid", Journal of Chemical Physics '''128''' 134508 (2008)]</ref>) | |||
:<math>P_c = 0.0228 + 0.0742 T_c</math> | |||
and (Eq. 4) | |||
:<math>\rho_c = 0.2534 + 0.071 \frac{1}{T_c}</math> | |||
The repulsive form of the potential has no [[Critical points | critical point]]. | |||
==Triple points== | |||
The [[triple point |triple points]] for this model have been studied by Azhar and co-workers | |||
<ref>[http://dx.doi.org/10.1063/1.481068 Fouad El Azhar, Marc Baus, Jean-Paul Ryckaert and Evert Jan Meijer "Line of triple points for the hard-core Yukawa model: A computer simulation study", Journal of Chemical Physics '''112''' pp. 5121- (2000)]</ref>. | |||
==Virial coefficients== | |||
For the attractive form of the potential the [[Virial equation of state |virial coefficients]] have been calculated by Naresh and Singh <ref>[http://dx.doi.org/10.1016/j.fluid.2009.06.019 D.J. Naresh and Jayant K. Singh "Virial coefficients of hard-core attractive Yukawa fluids", Fluid Phase Equilibria '''285''' pp. 36-43 (2009)]</ref>. | |||
==Liquid-vapour coexistence== | |||
<ref>[http://dx.doi.org/10.1063/1.3385894 E. B. El Mendoub, J.-F. Wax, and N. Jakse "Evolution of the liquid-vapor coexistence of the hard-core Yukawa fluid as a function of the interaction range", Journal of Chemical Physics '''132''' 164503 (2010)]</ref> | |||
==Surface tension== | |||
[[Surface tension]] <ref>[http://dx.doi.org/10.1063/1.3578637 G. Odriozola, M. Bárcenas, and P. Orea "Vapor–liquid surface tension of strong short-range Yukawa fluid", Journal of Chemical Physics '''134''' 154702 (2011)]</ref>. | |||
==Radial distribution function== | |||
[[Radial distribution function]]<ref>[http://dx.doi.org/10.1080/00268976.2010.505586 Douglas Henderson and Dezső Boda "Mean spherical approximation for the Yukawa fluid radial distribution function", Molecular Physics '''109''' pp. 1009-1013 (2011)]</ref> | |||
==Phase diagram== | ==Phase diagram== | ||
:'' | [[Phase diagrams | Phase diagram]] | ||
<ref>[http://dx.doi.org/10.1063/1.466781 Enrique Lomba and Noé G. Almarza "Role of the interaction range in the shaping of phase diagrams in simple fluids. The hard sphere Yukawa fluid as a case study", Journal of Chemical Physics '''100''' pp. 8367-8372 (1994)]</ref> | |||
<ref>[http://dx.doi.org/10.1063/1.467526 M. H. J. Hagen and D. Frenkel "Determination of phase diagrams for the hard-core attractive Yukawa system", Journal of Chemical Physics '''101''' pp. 4093-4097 (1994)]</ref> | |||
<ref>[http://dx.doi.org/10.1063/1.2743623 Yurko Duda, Ascención Romero-Martínez, and Pedro Orea "Phase diagram and surface tension of the hard-core attractive Yukawa model of variable range: Monte Carlo simulations", Journal of Chemical Physics '''126''' 224510 (2007)]</ref> | |||
<ref>[http://dx.doi.org/10.1063/1.2883694 Pedro Orea and Yurko Duda "On the corresponding states law of the Yukawa fluid", Journal of Chemical Physics '''128''' 134508 (2008)]</ref> | |||
==Density-functional theory== | |||
[[Density-functional theory]] <ref>[http://dx.doi.org/10.1063/1.4742154 Marius M. Hatlo, Priyanka Banerjee, Jan Forsman, and Leo Lue "Density functional theory for Yukawa fluids", Journal of Chemical Physics '''137''' 064115 (2012)]</ref>. | |||
==See also== | |||
*[[SALR potential]] | |||
*[[Soft sphere attractive Yukawa model]] | |||
==References== | ==References== | ||
<references/> | |||
'''Related reading''' | |||
*[http://dx.doi.org/10.1063/1.3281416 J. Torres-Arenas, L. A. Cervantes, A. L. Benavides, G. A. Chapela, and F. del Río "Discrete perturbation theory for the hard-core attractive and repulsive Yukawa potentials", Journal of Chemical Physics '''132''' 034501 (2010)] | |||
*[http://dx.doi.org/10.1063/1.3357352 Pedro Orea, Carlos Tapia-Medina, Davide Pini, and Albert Reiner "Thermodynamic properties of short-range attractive Yukawa fluid: Simulation and theory", Journal of Chemical Physics '''132''' 114108 (2010)] | |||
*[http://dx.doi.org/10.1063/1.3610400 Eun-Young Kim, Soon-Chul Kim, and Baek-Seok Seong "Structure and thermodynamics of hard-core Yukawa fluids: Thermodynamic perturbation approaches", Journal of Chemical Physics '''135''' 034505 (2011)] | |||
[[Category: Models]] | [[Category: Models]] |
Latest revision as of 14:00, 14 March 2018
The hard core Yukawa potential [1] has two forms, the attractive Yukawa potential:
and the repulsive form
where is the intermolecular pair potential, is the distance between site 1 and site 2, is the hard diameter, is the energy well depth (), and is a parameter that controls the interaction range ().
The repulsive form has been used to study charge-stabilised colloid-colloid interactions.
Critical point[edit]
For the attractive form of the potential, from a study of the law of corresponding states, one has (Eq. 3 in [2])
and (Eq. 4)
The repulsive form of the potential has no critical point.
Triple points[edit]
The triple points for this model have been studied by Azhar and co-workers [3].
Virial coefficients[edit]
For the attractive form of the potential the virial coefficients have been calculated by Naresh and Singh [4].
Liquid-vapour coexistence[edit]
Surface tension[edit]
Radial distribution function[edit]
Radial distribution function[7]
Phase diagram[edit]
Phase diagram [8] [9] [10] [11]
Density-functional theory[edit]
Density-functional theory [12].
See also[edit]
References[edit]
- ↑ J. S. Rowlinson "The Yukawa potential", Physica A: Statistical Mechanics and its Applications 156 pp. 15-34 (1989)
- ↑ Pedro Orea and Yurko Duda "On the corresponding states law of the Yukawa fluid", Journal of Chemical Physics 128 134508 (2008)
- ↑ Fouad El Azhar, Marc Baus, Jean-Paul Ryckaert and Evert Jan Meijer "Line of triple points for the hard-core Yukawa model: A computer simulation study", Journal of Chemical Physics 112 pp. 5121- (2000)
- ↑ D.J. Naresh and Jayant K. Singh "Virial coefficients of hard-core attractive Yukawa fluids", Fluid Phase Equilibria 285 pp. 36-43 (2009)
- ↑ E. B. El Mendoub, J.-F. Wax, and N. Jakse "Evolution of the liquid-vapor coexistence of the hard-core Yukawa fluid as a function of the interaction range", Journal of Chemical Physics 132 164503 (2010)
- ↑ G. Odriozola, M. Bárcenas, and P. Orea "Vapor–liquid surface tension of strong short-range Yukawa fluid", Journal of Chemical Physics 134 154702 (2011)
- ↑ Douglas Henderson and Dezső Boda "Mean spherical approximation for the Yukawa fluid radial distribution function", Molecular Physics 109 pp. 1009-1013 (2011)
- ↑ Enrique Lomba and Noé G. Almarza "Role of the interaction range in the shaping of phase diagrams in simple fluids. The hard sphere Yukawa fluid as a case study", Journal of Chemical Physics 100 pp. 8367-8372 (1994)
- ↑ M. H. J. Hagen and D. Frenkel "Determination of phase diagrams for the hard-core attractive Yukawa system", Journal of Chemical Physics 101 pp. 4093-4097 (1994)
- ↑ Yurko Duda, Ascención Romero-Martínez, and Pedro Orea "Phase diagram and surface tension of the hard-core attractive Yukawa model of variable range: Monte Carlo simulations", Journal of Chemical Physics 126 224510 (2007)
- ↑ Pedro Orea and Yurko Duda "On the corresponding states law of the Yukawa fluid", Journal of Chemical Physics 128 134508 (2008)
- ↑ Marius M. Hatlo, Priyanka Banerjee, Jan Forsman, and Leo Lue "Density functional theory for Yukawa fluids", Journal of Chemical Physics 137 064115 (2012)
Related reading
- J. Torres-Arenas, L. A. Cervantes, A. L. Benavides, G. A. Chapela, and F. del Río "Discrete perturbation theory for the hard-core attractive and repulsive Yukawa potentials", Journal of Chemical Physics 132 034501 (2010)
- Pedro Orea, Carlos Tapia-Medina, Davide Pini, and Albert Reiner "Thermodynamic properties of short-range attractive Yukawa fluid: Simulation and theory", Journal of Chemical Physics 132 114108 (2010)
- Eun-Young Kim, Soon-Chul Kim, and Baek-Seok Seong "Structure and thermodynamics of hard-core Yukawa fluids: Thermodynamic perturbation approaches", Journal of Chemical Physics 135 034505 (2011)