Ramp model: Difference between revisions

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m (→‎Repulsive Ramp Model: Slight tidy.)
 
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:<math>\rho_c \sigma^3  \simeq 0.380 \pm 0.002</math>
:<math>\rho_c \sigma^3  \simeq 0.380 \pm 0.002</math>
:<math>p_c^*/T_c^* \simeq 0.49 \pm 0.01</math>
:<math>p_c^*/T_c^* \simeq 0.49 \pm 0.01</math>
While this liquid-liquid critical point was long held to be in the stable region of the phase diagram, a high density double-network structure was found to be thermodynamically more stable than the high-density liquid under any conditions.<ref name="paraty">
[https://doi.org/10.1103/PhysRevLett.127.015701  A. P. Bartók, G. Hantal, L. B. Pártay "Insight into Liquid Polymorphism from the Complex Phase Behavior of a Simple Model", Physical Review Letters '''127''' 015701 (2021)]
</ref>:


== Repulsive Ramp Model ==
== Repulsive Ramp Model ==
In the repulsive ramp case, where <math> W_a = 0 </math>, neither liquid-vapor nor liquid-liquid stable equilibria occur
In the repulsive ramp case, where <math> W_a = 0 </math>, neither liquid-vapor nor liquid-liquid stable equilibria occur
<ref name="lomba"> reference to Lomba paper</ref>.  
<ref name="lomba"> </ref>.  
However, for this model a low density crystalline phase has been found.
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.
This solid phase presents re-entrant melting, i.e. this solid melts into the fluid phase as the pressure is increased.
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Ramp [[lattice gas|Lattice Gas]] model  
Ramp [[lattice gas|Lattice Gas]] model  
<ref>
<ref>
[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 ''iFirst'' (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)]
</ref>
</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
hard sphere]] model with exclusion of nearest neighbours of occupied positions plus a repulsive interaction
hard sphere]] model with exclusion of nearest neighbours of occupied positions plus a repulsive interaction
with next-to-nearest neighbours.
with next-to-nearest neighbours.
The potential energy of the system is then given by:
The total potential energy of the system is then given by:


:<math>
:<math>
U_{ij} = \epsilon \sum_{[ij]} S_i S_j
U = \epsilon \sum_{[ij]} S_i S_j
</math>
</math>


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==See also==
==See also==
*[[Triangular lattice ramp model]]
*[[Polyamorphism: Ramp model]]
*[[Polyamorphism: Ramp model]]
*[[Fermi-Jagla model]]
==References==
==References==
<references />
<references />
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*[http://dx.doi.org/10.1103/PhysRevE.74.031108 Limei Xu, Sergey V. Buldyrev, C. Austen Angell, and H. Eugene Stanley "Thermodynamics and dynamics of the two-scale spherically symmetric Jagla ramp model of anomalous liquids", Physical Review E '''74''' 031108 (2006)]
*[http://dx.doi.org/10.1103/PhysRevE.74.031108 Limei Xu, Sergey V. Buldyrev, C. Austen Angell, and H. Eugene Stanley "Thermodynamics and dynamics of the two-scale spherically symmetric Jagla ramp model of anomalous liquids", Physical Review E '''74''' 031108 (2006)]
*[http://dx.doi.org/10.1063/1.3043665 Limei Xu, Sergey V. Buldyrev, Nicolas Giovambattista, C. Austen Angell, and H. Eugene Stanley "A monatomic system with a liquid-liquid critical point and two distinct glassy states", Journal of Chemical Physics '''130''' 054505 (2009)]
*[http://dx.doi.org/10.1063/1.3043665 Limei Xu, Sergey V. Buldyrev, Nicolas Giovambattista, C. Austen Angell, and H. Eugene Stanley "A monatomic system with a liquid-liquid critical point and two distinct glassy states", Journal of Chemical Physics '''130''' 054505 (2009)]
*[http://dx.doi.org/10.3390/ijms11125184 Limei Xu, Sergey V. Buldyrev, Nicolas Giovambattista,  and H. Eugene Stanley "Liquid-Liquid Phase Transition and Glass Transition in a Monoatomic Model", International Journal of Molecular Sciences '''11''' pp. 5184-5200 (2010)]
*[http://dx.doi.org/10.1063/1.3521486 Limei Xu, Nicolas Giovambattista, Sergey V. Buldyrev, Pablo G. Debenedetti, and H. Eugene Stanley "Waterlike glass polyamorphism in a monoatomic isotropic Jagla model", Journal of Chemical Physics '''134''' 064507 (2011)]
*[http://dx.doi.org/10.1063/1.4921559 Jiayuan Luo, Limei Xu, C. Austen Angell, H. Eugene Stanley and Sergey V. Buldyrev "Physics of the Jagla model as the liquid-liquid coexistence line slope varies", Journal of Chemical Physics '''142''' 224501 (2015)]
[[Category:models]]
[[Category:models]]
[[category:Polyamorphic systems]]
[[category:Polyamorphic systems]]

Latest revision as of 23:20, 30 July 2021

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[edit]

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

and the liquid-liquid critical point:

While this liquid-liquid critical point was long held to be in the stable region of the phase diagram, a high density double-network structure was found to be thermodynamically more stable than the high-density liquid under any conditions.[3]:

Repulsive Ramp Model[edit]

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[edit]

Recently, similar behaviour has been found in a three-dimensional Repulsive Ramp Lattice Gas model [4] 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[edit]

References[edit]

Related literature