Restricted primitive model: Difference between revisions
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The '''restricted primitive model''' (RPM) consists of an | |||
equimolar (i.e. neutral)-equisized mixture of anions and cations which interact | |||
via the potential | |||
:<math> \Phi_{RPM}(r) = \Phi_{HS}(r)+ \frac{1}{4\pi\varepsilon_0} \frac{q_+q_-}{r} </math> | |||
where <math>\Phi_{HS}(r)</math> is the [[Hard sphere model| hard sphere potential]]. | |||
==See also== | |||
*[[Soft primitive model]] | |||
*[[Ultrasoft restricted primitive model]] | |||
==References== | ==References== | ||
<references/> | |||
;Related reading | |||
*[http://dx.doi.org/10.1063/1.1576374 Carlos Vega, José L. F. Abascal, Carl McBride and Fernando Bresme "The fluid–solid equilibrium for a charged hard sphere model revisited", Journal of Chemical Physics '''119''' pp. 964-971 (2003)] | |||
*[http://dx.doi.org/10.1103/PhysRevE.68.052501 José L. F. Abascal, Carlos Vega, Carl McBride and Fernando Bresme "Characterization of the order-disorder transition of a charged hard-sphere model", Physical Review E '''68''' 052501 (2003)] | |||
[[category:models]] | [[category:models]] | ||
[[category: mixtures]] | |||
Latest revision as of 16:05, 12 April 2016
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The restricted primitive model (RPM) consists of an equimolar (i.e. neutral)-equisized mixture of anions and cations which interact via the potential
where is the hard sphere potential.
See also[edit]
References[edit]
- Related reading
- Carlos Vega, José L. F. Abascal, Carl McBride and Fernando Bresme "The fluid–solid equilibrium for a charged hard sphere model revisited", Journal of Chemical Physics 119 pp. 964-971 (2003)
- José L. F. Abascal, Carlos Vega, Carl McBride and Fernando Bresme "Characterization of the order-disorder transition of a charged hard-sphere model", Physical Review E 68 052501 (2003)