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22 February 2007
- 16:1816:18, 22 February 2007 diff hist +4 m Widom-Rowlinson model No edit summary
- 16:1816:18, 22 February 2007 diff hist +1 m Widom-Rowlinson model →References
- 16:1716:17, 22 February 2007 diff hist +2 m Widom-Rowlinson model →References
- 16:1716:17, 22 February 2007 diff hist +121 m Widom-Rowlinson model →References
- 16:1316:13, 22 February 2007 diff hist +18 m Widom-Rowlinson model No edit summary
- 16:0916:09, 22 February 2007 diff hist +370 Nm Widom-Rowlinson model New page: The Widom-Rowlinson model for mixtures takes the form: <math> V \left( r_{ij} \right) = 0 </math> if <math> i </math> and <math> j</math> are particles of the same species <math> V \lef...
- 16:0316:03, 22 February 2007 diff hist +1 m Hard sphere model No edit summary
- 16:0216:02, 22 February 2007 diff hist +26 m Hard sphere model No edit summary
- 16:0016:00, 22 February 2007 diff hist +50 m Metropolis Monte Carlo →Advanced techniques
- 15:5815:58, 22 February 2007 diff hist +62 m Metropolis Monte Carlo No edit summary
- 14:5114:51, 22 February 2007 diff hist −6 m Flexible molecules →Van der Waals intramolecular interactions
- 13:5613:56, 22 February 2007 diff hist +63 m Models No edit summary
- 13:2013:20, 22 February 2007 diff hist −4 m Intermolecular Interactions →Site-site intermolecular potentials
- 13:1513:15, 22 February 2007 diff hist +1 m Intermolecular Interactions →Site-site intermolecular potentials
- 13:1413:14, 22 February 2007 diff hist +2 m Intermolecular Interactions No edit summary
- 13:1313:13, 22 February 2007 diff hist +79 m Intermolecular Interactions →Site-site intermolecular potentials
- 13:1113:11, 22 February 2007 diff hist +351 Nm Intermolecular Interactions New page: Most of the molecules cannot be modelled using spherical interactions. Different strategies have been used to represent the anisotropy of intermolecular interactions: == Site-site intermo...
- 12:5112:51, 22 February 2007 diff hist +15 m Flexible molecules →Bond Angles
- 12:5012:50, 22 February 2007 diff hist +90 m Flexible molecules →Bond distances
- 12:4612:46, 22 February 2007 diff hist +220 m Flexible molecules →Van der Waals intramolecular interactions
- 12:4312:43, 22 February 2007 diff hist +49 m Flexible molecules No edit summary
- 11:5411:54, 22 February 2007 diff hist +1 m Flexible molecules →Dihedral angles. Internal Rotation
- 11:5411:54, 22 February 2007 diff hist +15 m Flexible molecules →Dihedral angles. Internal Rotation
- 11:5111:51, 22 February 2007 diff hist +76 m Flexible molecules →Dihedral angles. Internal Rotation
- 11:4811:48, 22 February 2007 diff hist +960 m Flexible molecules →Dihedral angles. Internal Rotation
- 11:1611:16, 22 February 2007 diff hist +17 m Flexible molecules →Internal Rotation
- 11:1211:12, 22 February 2007 diff hist +129 m Flexible molecules No edit summary
21 February 2007
- 20:1220:12, 21 February 2007 diff hist +115 m Hard sphere model No edit summary
- 20:1020:10, 21 February 2007 diff hist 0 m 1-dimensional hard rods No edit summary
- 20:1020:10, 21 February 2007 diff hist +15 m 1-dimensional hard rods No edit summary
- 20:1020:10, 21 February 2007 diff hist +130 Nm 1-dimensional hard rods New page: Hard Rods, 1-dimensional system with ''hard sphere'' interactions. The statistical mechanics of this system can be solved exactly
- 20:0120:01, 21 February 2007 diff hist +108 m Van der Waals equation of state No edit summary
- 19:5819:58, 21 February 2007 diff hist +319 m Van der Waals equation of state No edit summary
- 19:4919:49, 21 February 2007 diff hist +479 Nm Van der Waals equation of state New page: The van der Waals equation is <math> \left. p = \frac{ n R T}{V - n b } - a \left( \frac{ n}{V} \right)^2 \right. </math>. where: * <math> p </math> is the pressure * <math> V </math> ...
- 18:5618:56, 21 February 2007 diff hist +124 m Metropolis Monte Carlo No edit summary
- 18:3318:33, 21 February 2007 diff hist +5 m Researchers and research groups →Spain
- 17:5917:59, 21 February 2007 diff hist +1 m Ideal gas No edit summary
- 17:5917:59, 21 February 2007 diff hist 0 m Ideal gas No edit summary
- 17:5717:57, 21 February 2007 diff hist −1 m Equations of state No edit summary
- 17:5617:56, 21 February 2007 diff hist +45 m Equations of state No edit summary
- 17:5417:54, 21 February 2007 diff hist +204 Nm Avogadro constant New page: The '''Avogadro constant''' (<math> N_A</math>) . Its value (in SI units, 2002 [http://www.codata.org/ CODATA] value) is: :<math> \left. N_A = 6.022 1415(10) \times 10^{23} mol^{-1}...
- 17:4717:47, 21 February 2007 diff hist +4 m Equation of State: Ideal Gas No edit summary
20 February 2007
- 17:2617:26, 20 February 2007 diff hist 0 m Isothermal-isobaric ensemble →References
- 17:2517:25, 20 February 2007 diff hist 0 m Isothermal-isobaric ensemble →References
- 17:2217:22, 20 February 2007 diff hist +460 m Isothermal-isobaric ensemble No edit summary
- 15:1515:15, 20 February 2007 diff hist +61 m Isothermal-isobaric ensemble No edit summary
- 15:1415:14, 20 February 2007 diff hist +39 Nm Isothermal-isobaric ensemble New page: In the Isothermal-Isobaric ensemble ...
- 15:0115:01, 20 February 2007 diff hist +1 m Virial coefficients of model systems No edit summary
- 12:4212:42, 20 February 2007 diff hist +360 m Virial coefficients of model systems No edit summary
- 11:3811:38, 20 February 2007 diff hist +222 Nm Virial coefficients of model systems New page: <math> \frac{p V}{N k_B T } = Z = 1 + \sum_{k=2} B_k(T) \rho^{k-1}. </math> where * <math> p </math> is the pressure *<math> V </math> is the volume *<math> N </math> is the number o...