Buckingham potential: Difference between revisions

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(New page: {{stub-general}} The '''Buckingham potential''' is given by :<math>\Phi_{12}(r) = A \exp \left(-Br\right) - \frac{C}{r^6}</math> ==References== category: models)
 
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:<math>\Phi_{12}(r) = A \exp \left(-Br\right) - \frac{C}{r^6}</math>
:<math>\Phi_{12}(r) = A \exp \left(-Br\right) - \frac{C}{r^6}</math>
==References==
==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]]
[[category: models]]

Revision as of 12:51, 8 February 2008

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The Buckingham potential is given by

References

  1. 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)