Hard core Yukawa potential: Difference between revisions
Carl McBride (talk | contribs) m (Added a reference) |
Carl McBride (talk | contribs) m (Added critical point data.) |
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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 12:33, 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, 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 } is the energy well depth (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 > 0 } ), 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 (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \rho _{c}=0.2534+0.071{\frac {1}{T_{c}}}} .
The repulsive form of the potential has no critical point.
Triple points
Phase diagram
- Main article: Phase diagram of the Yukawa potential