Hard core Yukawa potential: Difference between revisions

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==Liquid-vapour coexistence==
==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>
<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>.
==Phase diagram==
==Phase diagram==
:''Main article: [[Phase diagram of the Yukawa potential]]''
:''Main article: [[Phase diagram of the Yukawa potential]]''

Revision as of 17:48, 18 April 2011

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

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

The triple points for this model have been studied by Azhar and co-workers [3].

Virial coefficients

For the attractive form of the potential the virial coefficients have been calculated by Naresh and Singh [4].

Liquid-vapour coexistence

[5]

Surface tension

Surface tension [6].

Phase diagram

Main article: Phase diagram of the Yukawa potential

Two-term Yukawa potentials

Both the attractive and the repulsive form have been combined to produce the hard-sphere plus two Yukawa potential (H2Y) [7].

References

Related reading