Modified Lennard-Jones model: Difference between revisions
		
		
		
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| Carl McBride (talk | contribs) m (typo) | Carl McBride (talk | contribs)   (Added note that both C3 and C4 should be negative.) | ||
| Line 15: | Line 15: | ||
| <math>C_4 = 0.083312 \epsilon</math>   | <math>C_4 = 0.083312 \epsilon</math>   | ||
| and <math>C_5 = 0.74689\epsilon</math>. These parametrs are chosen so that the function <math>\Phi_{12}(r)</math>, as well as the first derivative, is continuous both at <math>r = 2.3\sigma</math> and <math>r = 2.5\sigma</math>. | and <math>C_5 = 0.74689\epsilon</math>. These parametrs are chosen so that the function <math>\Phi_{12}(r)</math>, as well as the first derivative, is continuous both at <math>r = 2.3\sigma</math> and <math>r = 2.5\sigma</math>. | ||
| These parameters have recently been recalculated by Asano and Fuchizaki <ref>[http://dx.doi.org/10.1063/1.4764855  Yuta Asano and Kazuhiro Fuchizaki "Phase diagram of the modified Lennard-Jones system", Journal of Chemical Physics '''137''' 174502 (2012)]</ref>, leading to | These parameters have recently been recalculated with greater precision by Asano and Fuchizaki <ref>[http://dx.doi.org/10.1063/1.4764855  Yuta Asano and Kazuhiro Fuchizaki "Phase diagram of the modified Lennard-Jones system", Journal of Chemical Physics '''137''' 174502 (2012)]</ref>, leading to | ||
| <math>C_1 = 0.0163169237\epsilon</math>,   | <math>C_1 = 0.0163169237\epsilon</math>,   | ||
| <math>C_2 = 3136.5686  \epsilon</math>   | <math>C_2 = 3136.5686  \epsilon</math>   | ||
| <math>C_3 = 68.069 \epsilon</math>   | <math>C_3 = 68.069 \epsilon</math>   | ||
| <math>C_4 =  −0.0833111261\epsilon</math>   | <math>C_4 =  −0.0833111261\epsilon</math>   | ||
| and <math>C_5 = 0.746882273 \epsilon</math>. | and <math>C_5 = 0.746882273 \epsilon</math>. Note however, that it seems that '''both''' <math>C_3</math> and <math>C_4</math> should be negative for these parameters to work. | ||
| ==References== | ==References==   | ||
| <references/> | <references/> | ||
| [[category: models]] | [[category: models]] | ||
Revision as of 18:18, 7 November 2012
The modified Lennard-Jones model is given by (Eq. 2 [1]):
where , and . These parametrs are chosen so that the function , as well as the first derivative, is continuous both at and . These parameters have recently been recalculated with greater precision by Asano and Fuchizaki [2], leading to , Failed to parse (syntax error): {\displaystyle C_4 = −0.0833111261\epsilon} and . Note however, that it seems that both and should be negative for these parameters to work.
References
- ↑ Jeremy Q. Broughton and George H. Gilmer "Molecular dynamics investigation of the crystal–fluid interface. I. Bulk properties", Journal of Chemical Physics 79 pp. 5095-5104 (1983)
- ↑ Yuta Asano and Kazuhiro Fuchizaki "Phase diagram of the modified Lennard-Jones system", Journal of Chemical Physics 137 174502 (2012)