Buckingham potential: Difference between revisions

Revision as of 15:02, 17 July 2008

The Buckingham potential is given by

\Phi _{12}(r)=A\exp \left(-Br\right)-{\frac {C}{r^{6}}}

where $\Phi _{12}(r)$ is the intermolecular pair potential, $r:=|\mathbf {r} _{1}-\mathbf {r} _{2}|$ , and $A$ , $B$ and $C$ are constants.

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 :<math>\Phi_{12}(r) = A \exp \left(-Br\right) - \frac{C}{r^6}</math>
+where <math>\Phi_{12}(r)</math> is the [[intermolecular pair potential]], <math>r := |\mathbf{r}_1 - \mathbf{r}_2|</math>, and <math>A</math>, <math>B</math> and <math>C</math> are constants.
 ==References==
 #[http://dx.doi.org/10.1098/rspa.1938.0173 R. A. Buckingham "The Classical Equation of State of Gaseous Helium, Neon and Argon", Proceedings of the Royal Society of London. Series A, Mathematical and Physical Sciences '''168''' pp. 264-283 (1938)]
 [[category: models]]