Gaussian overlap model: Difference between revisions

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*[http://dx.doi.org/10.1021/j100238a030 P. A. Monson and K. E. Gubbins "Equilibrium properties of the Gaussian overlap fluid. Monte Carlo simulation and thermodynamic perturbation theory" Journal of Physical Chemistry '''87''' pp. 2852-2858 (1983)]
*[http://dx.doi.org/10.1021/j100238a030 P. A. Monson and K. E. Gubbins "Equilibrium properties of the Gaussian overlap fluid. Monte Carlo simulation and thermodynamic perturbation theory" Journal of Physical Chemistry '''87''' pp. 2852-2858 (1983)]
*[http://dx.doi.org/10.1080/00268978900101841 Tomas Boublik "The gaussian overlap model again", Molecular Physics '''67''' pp. 1327-1336 (1989)]
*[http://dx.doi.org/10.1080/00268978900101841 Tomas Boublik "The gaussian overlap model again", Molecular Physics '''67''' pp. 1327-1336 (1989)]
*[http://dx.doi.org/10.1063/1.3429354 Lindsey Ann Shall and S. A. Egorov "Structural and dynamical anomalies of a Gaussian core fluid: A mode-coupling theory study", Journal of Chemical Physics '''132''' 184504 (2010)]


[[Category: Models]]
[[Category: Models]]

Revision as of 11:22, 12 May 2010

The Gaussian overlap model was developed by Bruce J. Berne and Philip Pechukas [1]and is given by Eq. 3 in the aforementioned reference:

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \Phi_{12}(\mathbf{u}_1,\mathbf{u}_2,\mathbf{r}) = \epsilon(\mathbf{u}_1,\mathbf{u}_2) \exp \left[ \frac{-r}{\sigma (\mathbf{u}_1,\mathbf{u}_2, \hat{\mathbf{r}}) } \right]^n}

where Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle n=2} , is the intermolecular pair potential, Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \epsilon(\mathbf{u}_1,\mathbf{u}_2) } and Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \sigma (\mathbf{u}_1,\mathbf{u}_2, \hat{\mathbf{r}})} are angle dependent strength and range parameters, and Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \hat{\mathbf{r}}} is a unit vector. Not long after the introduction of the Gaussian overlap model Stillinger [2] proposed a stripped-down version of the model, known as the Gaussian core model. Note that as Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle n \rightarrow \infty} this potential becomes the penetrable sphere model.

Equation of state

Main article: Equations of state for the Gaussian overlap model

Virial coefficients

Main article: Gaussian overlap model: virial coefficients

Phase diagram

The phase diagram of the Gaussian-core model has been calculated by Prestipino et al.[3] while the solid-liquid phase equilibria has been calculated by Mausbach et al [4] using the GWTS algorithm.

Shear viscosity

[5]

References

Related reading