Buckingham potential: Difference between revisions
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Carl McBride (talk | contribs) (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
- 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 \Phi_{12}(r) = A \exp \left(-Br\right) - \frac{C}{r^6}}