10-4-3 Lennard-Jones potential: Difference between revisions
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Carl McBride (talk | contribs) m (New page: {{Stub-general}} The '''10-4-3''' model is a variant of the Lennard-Jones model designed for use in fluid-wall systems : <math> \Phi_{W} \left( x \right) = 2\pi \epsilon_{sf} \rho_s...) |
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Revision as of 15:47, 9 October 2007
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The 10-4-3 model is a variant of the Lennard-Jones model designed for use in fluid-wall systems
![{\displaystyle \Phi _{W}\left(x\right)=2\pi \epsilon _{sf}\rho _{s}\sigma ^{2}\Delta \left[{\frac {2}{5}}\left({\frac {\sigma }{x}}\right)^{10}-\left({\frac {\sigma }{x}}\right)^{4}-\left({\frac {\sigma ^{4}}{3\Delta (x+0.61\Delta )^{3}}}\right)\right]}](https://wikimedia.org/api/rest_v1/media/math/render/svg/3242e99ee332ed9d01f54e69323f6912928eaaf9)
See also
References
- William A. Steele "The physical interaction of gases with crystalline solids I. Gas-solid energies and properties of isolated adsorbed atoms", Surface Science 36 pp. 317-352 (1973)
- William A. Steele "The interaction of rare gas atoms with graphitized carbon black", Journal of Physical Chemistry 82 pp. 817 - 821 (1978)