User contributions for Noe
Jump to navigation
Jump to search
22 February 2007
- 17:0917:09, 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...
- 17:0317:03, 22 February 2007 diff hist +1 m Hard sphere model No edit summary
- 17:0217:02, 22 February 2007 diff hist +26 m Hard sphere model No edit summary
- 17:0017:00, 22 February 2007 diff hist +50 m Metropolis Monte Carlo →Advanced techniques
- 16:5816:58, 22 February 2007 diff hist +62 m Metropolis Monte Carlo No edit summary
- 15:5115:51, 22 February 2007 diff hist −6 m Flexible molecules →Van der Waals intramolecular interactions
- 14:5614:56, 22 February 2007 diff hist +63 m Models No edit summary
- 14:2014:20, 22 February 2007 diff hist −4 m Intermolecular Interactions →Site-site intermolecular potentials
- 14:1514:15, 22 February 2007 diff hist +1 m Intermolecular Interactions →Site-site intermolecular potentials
- 14:1414:14, 22 February 2007 diff hist +2 m Intermolecular Interactions No edit summary
- 14:1314:13, 22 February 2007 diff hist +79 m Intermolecular Interactions →Site-site intermolecular potentials
- 14:1114:11, 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...
- 13:5113:51, 22 February 2007 diff hist +15 m Flexible molecules →Bond Angles
- 13:5013:50, 22 February 2007 diff hist +90 m Flexible molecules →Bond distances
- 13:4613:46, 22 February 2007 diff hist +220 m Flexible molecules →Van der Waals intramolecular interactions
- 13:4313:43, 22 February 2007 diff hist +49 m Flexible molecules No edit summary
- 12:5412:54, 22 February 2007 diff hist +1 m Flexible molecules →Dihedral angles. Internal Rotation
- 12:5412:54, 22 February 2007 diff hist +15 m Flexible molecules →Dihedral angles. Internal Rotation
- 12:5112:51, 22 February 2007 diff hist +76 m Flexible molecules →Dihedral angles. Internal Rotation
- 12:4812:48, 22 February 2007 diff hist +960 m Flexible molecules →Dihedral angles. Internal Rotation
- 12:1612:16, 22 February 2007 diff hist +17 m Flexible molecules →Internal Rotation
- 12:1212:12, 22 February 2007 diff hist +129 m Flexible molecules No edit summary
21 February 2007
- 21:1221:12, 21 February 2007 diff hist +115 m Hard sphere model No edit summary
- 21:1021:10, 21 February 2007 diff hist 0 m 1-dimensional hard rods No edit summary
- 21:1021:10, 21 February 2007 diff hist +15 m 1-dimensional hard rods No edit summary
- 21:1021:10, 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
- 21:0121:01, 21 February 2007 diff hist +108 m Van der Waals equation of state No edit summary
- 20:5820:58, 21 February 2007 diff hist +319 m Van der Waals equation of state No edit summary
- 20:4920:49, 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> ...
- 19:5619:56, 21 February 2007 diff hist +124 m Metropolis Monte Carlo No edit summary
- 19:3319:33, 21 February 2007 diff hist +5 m Researchers and research groups →Spain
- 18:5918:59, 21 February 2007 diff hist +1 m Ideal gas No edit summary
- 18:5918:59, 21 February 2007 diff hist 0 m Ideal gas No edit summary
- 18:5718:57, 21 February 2007 diff hist −1 m Equations of state No edit summary
- 18:5618:56, 21 February 2007 diff hist +45 m Equations of state No edit summary
- 18:5418:54, 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}...
- 18:4718:47, 21 February 2007 diff hist +4 m Equation of State: Ideal Gas No edit summary
20 February 2007
- 18:2618:26, 20 February 2007 diff hist 0 m Isothermal-isobaric ensemble →References
- 18:2518:25, 20 February 2007 diff hist 0 m Isothermal-isobaric ensemble →References
- 18:2218:22, 20 February 2007 diff hist +460 m Isothermal-isobaric ensemble No edit summary
- 16:1516:15, 20 February 2007 diff hist +61 m Isothermal-isobaric ensemble No edit summary
- 16:1416:14, 20 February 2007 diff hist +39 Nm Isothermal-isobaric ensemble New page: In the Isothermal-Isobaric ensemble ...
- 16:0116:01, 20 February 2007 diff hist +1 m Virial coefficients of model systems No edit summary
- 13:4213:42, 20 February 2007 diff hist +360 m Virial coefficients of model systems No edit summary
- 12:3812:38, 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...
19 February 2007
- 20:5520:55, 19 February 2007 diff hist +28 m Canonical ensemble →Partition Function
- 20:5420:54, 19 February 2007 diff hist +23 m Canonical ensemble →[[Helmholtz energy function|Free energy]]
- 20:5220:52, 19 February 2007 diff hist +134 m Canonical ensemble →[[Helmholtz energy function|free energy]]
- 20:5020:50, 19 February 2007 diff hist 0 m Canonical ensemble →[[Free energy|Helmholtz energy function]]
- 20:4920:49, 19 February 2007 diff hist +26 m Canonical ensemble →[[Free energy]]
- 20:4720:47, 19 February 2007 diff hist +23 m Canonical ensemble No edit summary
- 20:4620:46, 19 February 2007 diff hist +170 m Canonical ensemble →Partition Function
- 20:4220:42, 19 February 2007 diff hist +224 m Canonical ensemble →Partition Function
- 20:3320:33, 19 February 2007 diff hist +64 m Canonical ensemble →Partition Function
- 20:3220:32, 19 February 2007 diff hist +37 m Canonical ensemble →Partition Function
- 20:2520:25, 19 February 2007 diff hist −2 m Canonical ensemble →Partition Function
- 20:2520:25, 19 February 2007 diff hist −10 m Canonical ensemble →Partition Function
- 20:2020:20, 19 February 2007 diff hist +140 m Canonical ensemble →Partition Function
- 20:1720:17, 19 February 2007 diff hist −5 m Canonical ensemble No edit summary
- 20:1620:16, 19 February 2007 diff hist +246 Nm Canonical ensemble New page: Canonical Ensemble: Variables: * Number of Particles, <math> N </math> * Volume, <math> V </math> * Temperature, <math> T </math> == == == Partition Function == ''Classical'' Partiti...
- 20:0920:09, 19 February 2007 diff hist +42 m Main Page No edit summary
- 20:0120:01, 19 February 2007 diff hist +2 m Metropolis Monte Carlo →Temperature
- 19:5219:52, 19 February 2007 diff hist +1 m Metropolis Monte Carlo →Temperature
- 19:4819:48, 19 February 2007 diff hist +9 m Metropolis Monte Carlo →Temperature
- 19:4719:47, 19 February 2007 diff hist 0 m Metropolis Monte Carlo No edit summary
- 19:4419:44, 19 February 2007 diff hist +108 m Metropolis Monte Carlo →Temperature
- 19:4319:43, 19 February 2007 diff hist +147 m Metropolis Monte Carlo →Temperature
- 19:4119:41, 19 February 2007 diff hist +18 m Metropolis Monte Carlo No edit summary
- 19:3919:39, 19 February 2007 diff hist +263 m Metropolis Monte Carlo No edit summary
- 19:2119:21, 19 February 2007 diff hist +18 m Metropolis Monte Carlo No edit summary
- 19:2019:20, 19 February 2007 diff hist +308 Nm Metropolis Monte Carlo New page: '''Metropolis Monte Carlo (MMC) ''' MMC Simulations can be carried out in different ensembles. For the case of one-component systems the usual ensembles are: * Canonical ensemble (<math>...
- 13:5613:56, 19 February 2007 diff hist −2 m Hard core Yukawa potential No edit summary
16 February 2007
- 20:2220:22, 16 February 2007 diff hist +2 m Carnahan-Starling equation of state →References
- 20:2120:21, 16 February 2007 diff hist −16 m Carnahan-Starling equation of state No edit summary
- 20:2020:20, 16 February 2007 diff hist −6 m Carnahan-Starling equation of state →References
- 20:1920:19, 16 February 2007 diff hist +80 m Carnahan-Starling equation of state →References
- 20:1320:13, 16 February 2007 diff hist +18 m Carnahan-Starling equation of state No edit summary
- 20:0620:06, 16 February 2007 diff hist −3 m Hard sphere model No edit summary
- 20:0620:06, 16 February 2007 diff hist +65 m Hard sphere model No edit summary
- 20:0420:04, 16 February 2007 diff hist +26 m Carnahan-Starling equation of state No edit summary
- 20:0220:02, 16 February 2007 diff hist +55 m Carnahan-Starling equation of state No edit summary
- 19:5919:59, 16 February 2007 diff hist +472 m Carnahan-Starling equation of state No edit summary
- 19:5019:50, 16 February 2007 diff hist +40 m Carnahan-Starling equation of state No edit summary
- 19:4919:49, 16 February 2007 diff hist +100 Nm Carnahan-Starling equation of state New page: The equation of Carnahan-Starling is an approxiamate equation of state for the Hard Sphere model
- 19:0319:03, 16 February 2007 diff hist 0 m Models No edit summary
- 19:0319:03, 16 February 2007 diff hist 0 m Square well model Square Well moved to Square well
- 19:0219:02, 16 February 2007 diff hist 0 m Models No edit summary
- 19:0119:01, 16 February 2007 diff hist 0 m Models No edit summary
- 18:5718:57, 16 February 2007 diff hist +27 m Lennard-Jones model No edit summary
- 18:5618:56, 16 February 2007 diff hist +373 m Lennard-Jones model No edit summary
- 18:4018:40, 16 February 2007 diff hist +58 m Square well model No edit summary
- 18:3518:35, 16 February 2007 diff hist +128 m Hard sphere model No edit summary
- 18:2318:23, 16 February 2007 diff hist +24 m Hyper-netted chain No edit summary
- 18:1618:16, 16 February 2007 diff hist +63 Lennard-Jones model No edit summary
- 17:3417:34, 16 February 2007 diff hist +1 Lennard-Jones model minor correction
- 17:3417:34, 16 February 2007 diff hist +149 Lennard-Jones model No edit summary
- 17:2717:27, 16 February 2007 diff hist +81 N Lennard-Jones model New page: Lennard-Jones Potential: V(r) = 4 ε [ (σ/r)**12 - (σ/r)**6 ]
- 13:1513:15, 16 February 2007 diff hist 0 Square well model small correction
- 13:1513:15, 16 February 2007 diff hist +305 N Square well model New page: Square well model: V(r) = ∞ , if r < σ V(r) = - ε , if σ ≤ r < λ σ V(r) = 0; if r ≤ λ σ where V(r) is the potential e...
- 12:5312:53, 16 February 2007 diff hist +14 m Hard sphere model correction of symbols