Hard core Yukawa potential: Difference between revisions

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The repulsive form has been used to study charge-stabilised [[Colloids |colloid-colloid]] interactions.  
The repulsive form has been used to study charge-stabilised [[Colloids |colloid-colloid]] interactions.  
==Critical point==
==Critical point==
For the attractive form of the potential, from a study of the [[law of corresponding states]], one has (Ref. 1 Eq. 3)
:<math>P_c = 0.0228 + 0.0742 T_c</math>
and (Ref. 1 Eq. 4)
:<math>\rho_c = 0.2534 + 0.071 \frac{1}{T_c}</math>.
The repulsive form of the potential has no critical point.  
The repulsive form of the potential has no critical point.  
==Triple points==
==Triple points==
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:''Main article: [[Phase diagram of the Yukawa potential]]''
:''Main article: [[Phase diagram of the Yukawa potential]]''
==References==
==References==
#[http://dx.doi.org/10.1063/1.2883694 Pedro Orea and Yurko Duda "On the corresponding states law of the Yukawa fluid",  Journal of Chemical Physics '''128''' 134508 (2008)]
[[Category: Models]]
[[Category: Models]]

Revision as of 13:33, 7 April 2008

The hard core Yukawa potential has two forms, the attractive Yukawa potential:

and the repulsive form

Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \Phi \left(r\right)=\left\{{\begin{array}{lll}\infty &;&r<\sigma \\\left({\frac {\epsilon \sigma }{r}}\right)\exp \left[-\kappa \left({\frac {r}{\sigma }}-1\right)\right]&;&r\geq \sigma \end{array}}\right.}

where is the intermolecular pair potential, is the distance, is the hard diameter, is the energy well depth (), 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 \kappa } is a parameter that controls the interaction range (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 \kappa > 0 } ).

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 (Ref. 1 Eq. 3)

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 P_c = 0.0228 + 0.0742 T_c}

and (Ref. 1 Eq. 4)

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 \rho_c = 0.2534 + 0.071 \frac{1}{T_c}} .

The repulsive form of the potential has no critical point.

Triple points

  1. Fouad El Azhar, Marc Baus, Jean-Paul Ryckaert and Evert Jan Meijer "Line of triple points for the hard-core Yukawa model: A computer simulation study", Journal of Chemical Physics 112 pp. 5121- (2000)

Phase diagram

Main article: Phase diagram of the Yukawa potential

References

  1. Pedro Orea and Yurko Duda "On the corresponding states law of the Yukawa fluid", Journal of Chemical Physics 128 134508 (2008)