C60: Difference between revisions

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where <math>N</math> is the number of atoms on each sphere, i.e. N=60.
where <math>N</math> is the number of atoms on each sphere, i.e. N=60.
====Approximate non-conformal potential====
The [[Approximate non-conformal potential]] ('''ANC''') for the C60 fullerene is given by (Eq 6 in <ref>[http://dx.doi.org/10.1016/j.chemphys.2017.05.014 Jesús Eloy Ramos "Effective intermolecular potential and critical point for C60 molecule", Chemical Physics '''492''' pp. 5-11 (2017)]</ref>):
:<math>\Phi_{12}(z) =  \epsilon \left[ \frac{1-a}{(z^3/S +1 - 1/S)^{1/3} -a} \right]^{12} - 2\epsilon \left[ \frac{1-a}{(z^3/S +1 - 1/S)^{1/3} -a} \right]^{6} </math>
where
* <math>z := r/r_m</math>
* <math>r_m</math> = 1.0281 nm
* <math> a </math> = 0.09574 is the hard-core diameter in units of <math>r_m</math>
* <math> \epsilon </math> = 3297.28 K is the well depth
* <math>S</math> = 0.4120 is a softness parameter
==Phase diagram==
==Phase diagram==
<ref>[http://dx.doi.org/10.1103/PhysRevLett.71.1200      Ailan Cheng, Michael L. Klein and Carlo Caccamo "Prediction of the phase diagram of rigid C60 molecules", Physical Review Letters '''71''' pp. 1200-1203 (1993)]</ref>
<ref>[http://dx.doi.org/10.1103/PhysRevLett.71.1200      Ailan Cheng, Michael L. Klein and Carlo Caccamo "Prediction of the phase diagram of rigid C60 molecules", Physical Review Letters '''71''' pp. 1200-1203 (1993)]</ref>
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*[http://dx.doi.org/10.1063/1.473192 C. Caccamo, D. Costa, and A. Fucile "A Gibbs ensemble Monte Carlo study of phase coexistence in model C60", Journal of Chemical Physics '''106''' pp.  255- (1997)]
*[http://dx.doi.org/10.1063/1.473192 C. Caccamo, D. Costa, and A. Fucile "A Gibbs ensemble Monte Carlo study of phase coexistence in model C60", Journal of Chemical Physics '''106''' pp.  255- (1997)]
*[http://dx.doi.org/10.1080/00268970902881979 M. Bahaa Khedr,  S. M. Osman and M.S. Al Busaidi "Surface tension, shear viscosity and isothermal compressibility of liquid C60 along the liquid-vapour coexistence", Molecular Physics '''107''' pp. 1355-1366 (2009)]
*[http://dx.doi.org/10.1080/00268970902881979 M. Bahaa Khedr,  S. M. Osman and M.S. Al Busaidi "Surface tension, shear viscosity and isothermal compressibility of liquid C60 along the liquid-vapour coexistence", Molecular Physics '''107''' pp. 1355-1366 (2009)]
*[http://dx.doi.org/10.1063/1.4866451  Minkyu Kim, Jaeeon Chang and Stanley I. Sandler "Monte Carlo simulations for the free energies of C60 and C70 fullerene crystals by acceptance ratio method and expanded ensemble method", Journal of Chemical Physics '''140''' 084110 (2014)]
*[http://dx.doi.org/10.1063/1.4932591  D. M. Edmunds, P. Tangney, D. D. Vvedensky and W. M. C. Foulkes "Free-energy coarse-grained potential for C60", Journal of Chemical Physics '''143''' 164509 (2015)]




[[category: models]]
[[category: models]]
[[category: Contains Jmol]]
[[category: Contains Jmol]]

Latest revision as of 19:01, 3 January 2018

C60, also known as Buckminsterfullerene is composed of carbon atoms.


<jmol>

 <jmolApplet>
 <script>set spin X 10; spin on</script>
 <size>200</size>
 <color>lightgrey</color>
   <wikiPageContents>C60.pdb</wikiPageContents>
</jmolApplet>
</jmol>
C60

Models[edit]

Girifalco potential[edit]

The Girifalco intermolecular pair potential is given by [1] (Eq. 4):

where

where is the number of atoms on each sphere, i.e. N=60.

Approximate non-conformal potential[edit]

The Approximate non-conformal potential (ANC) for the C60 fullerene is given by (Eq 6 in [2]):

where

  • = 1.0281 nm
  • = 0.09574 is the hard-core diameter in units of
  • = 3297.28 K is the well depth
  • = 0.4120 is a softness parameter

Phase diagram[edit]

[3] [4] [5] [6]

Liquid phase[edit]

[7]

Gel phase[edit]

Simulations of the Girifalco potential indicate a possible gel composed solely of C60 molecules [8]

References[edit]

Related reading