Triangular well model: Difference between revisions

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and λ > 1.
and λ > 1.
==Equation of state==
==Equation of state==
:''Main article: [[Equations of state for the triangular well model]]''
<ref>[http://dx.doi.org/10.1016/S0378-4371(00)00232-6  J. Largo and J. R. Solana "A simplified perturbation theory for equilibrium properties of triangular-well fluids", Physica A '''284''' pp. 68-78 (2000)]</ref>
<ref>[http://dx.doi.org/10.1080/00268976.2010.538738 Mustafa Koyuncu "Equation of state of a long-range triangular-well fluid", Molecular Physics '''109''' pp. 565-573 (2011)]</ref>
==Virial coefficients==
==Virial coefficients==
<math>B_2</math>, <math>B_3</math> <ref>[http://dx.doi.org/10.1063/1.1725746  M. J. Feinberg and Andrew G. De Rocco "Intermolecular Forces: The Triangle Well and Some Comparisons with the Square Well and Lennard-Jones", Journal of Chemical Physics '''41''' pp. 3439-3450 (1964)]</ref>
<math>B_2</math>, <math>B_3</math> <ref>[http://dx.doi.org/10.1063/1.1725746  M. J. Feinberg and Andrew G. De Rocco "Intermolecular Forces: The Triangle Well and Some Comparisons with the Square Well and Lennard-Jones", Journal of Chemical Physics '''41''' pp. 3439-3450 (1964)]</ref>

Revision as of 17:05, 19 February 2011

The triangular well model, proposed by T. Nagayimain one dimension [1][2], is given by

where is the intermolecular pair potential, is the distance , is the hard diameter, is the well depth and λ > 1.

Equation of state

[3] [4]

Virial coefficients

, [5] [6] and [7]

Critical point

Solid phase

[8]

References

Related reading