Ramp model: Difference between revisions

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m (→‎Lattice gas version: refererence updated)
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Ramp [[lattice gas|Lattice Gas]] model  
Ramp [[lattice gas|Lattice Gas]] model  
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[http://dx.doi.org/10.1080/00268970902729269  Johan Skule Hoye,  Enrique Lomba, and  Noe Garcia Almarza, "One- and three-dimensional lattice models with two repulsive ranges: simple systems with complex phase behaviour",  Molecular Physics 107, 321-330 (2009)]
[http://dx.doi.org/10.1080/00268970902729269  Johan Skule Hoye,  Enrique Lomba, and  Noe Garcia Almarza, "One- and three-dimensional lattice models with two repulsive ranges: simple systems with complex phase behaviour",  Molecular Physics '''107''', 321-330 (2009)]
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</ref>
The system is defined on a simple cubic lattice. The interaction is that of a [[lattice hard spheres|lattice
The system is defined on a simple cubic lattice. The interaction is that of a [[lattice hard spheres|lattice

Revision as of 11:39, 21 May 2009

The ramp model, proposed by Jagla [1] and sometimes known as the Jagla model, is described by:

where is the intermolecular pair potential, , and .

Graphically, one has:

where the red line represents an attractive implementation of the model, and the green line a repulsive implementation.

Critical points

For the particular case , the liquid-vapour critical point is located at [2]:

and the liquid-liquid critical point:

Repulsive Ramp Model

In the repulsive ramp case, where , neither liquid-vapor nor liquid-liquid stable equilibria occur [2]. However, for this model a low density crystalline phase has been found. This solid phase presents re-entrant melting, i.e. this solid melts into the fluid phase as the pressure is increased.

Lattice gas version

Recently, similar behaviour has been found in a three-dimensional Repulsive Ramp Lattice Gas model [3] The system is defined on a simple cubic lattice. The interaction is that of a lattice hard sphere model with exclusion of nearest neighbours of occupied positions plus a repulsive interaction with next-to-nearest neighbours. The total potential energy of the system is then given by:

where  ; refers to all the pairs of sites that are second neighbors, and indicates the occupation of site (0 indicates an empty site, 1 indicates an occupied site).

See also

References

Related literature