Hard dumbbell model: Difference between revisions

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{{Stub-general}}
[[Image:dumbell_peagreen.png|thumb|right|Representation of a tangential dumbbell model]]
The '''Hard dumbbell model''' consists of two [[hard sphere model |hard spheres]] separated by a distance <math>L</math>.
==Equation of state==
:''Main article: [[Equation of State: three-dimensional hard dumbbells | Equation of state for the hard dumbbell model]]''
==See also==
*[[Asymmetric hard dumbbell model]]
==References==
#[http://dx.doi.org/10.1063/1.1748236 A. Isihara "Theory of High Polymer Solutions (The Dumbbell Model)", Journal of Chemical Physics '''19''' pp. 397- (1951)]
;Related reading
*[http://dx.doi.org/10.1063/1.3528222  Ran Ni  and Marjolein Dijkstra "Crystal nucleation of colloidal hard dumbbells", Journal of Chemical Physics '''134''' 034501 (2011)]
==External resources==
*[ftp://ftp.dl.ac.uk/ccp5/ALLEN_TILDESLEY/F.16  Hard dumb-bell Monte Carlo program] sample FORTRAN computer code from the book [http://www.oup.com/uk/catalogue/?ci=9780198556459 M. P. Allen and D. J. Tildesley "Computer Simulation of Liquids", Oxford University Press (1989)].
[[Category: Models]]

Latest revision as of 16:30, 19 September 2012

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Representation of a tangential dumbbell model

The Hard dumbbell model consists of two hard spheres separated by a distance .

Equation of state[edit]

Main article: Equation of state for the hard dumbbell model

See also[edit]

References[edit]

  1. A. Isihara "Theory of High Polymer Solutions (The Dumbbell Model)", Journal of Chemical Physics 19 pp. 397- (1951)
Related reading

External resources[edit]