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19 March 2007
- 20:3820:38, 19 March 2007 diff hist −1 m Building up a face centered cubic lattice No edit summary
- 20:3520:35, 19 March 2007 diff hist +47 m Building up a simple cubic lattice →Atomic position(s) on a cubic cell
- 20:3420:34, 19 March 2007 diff hist +157 m Building up a simple cubic lattice No edit summary
- 19:4419:44, 19 March 2007 diff hist +42 m Lattice Structures →3-dimensional systems
- 19:3119:31, 19 March 2007 diff hist +13 m Building up a face centered cubic lattice No edit summary
- 19:1819:18, 19 March 2007 diff hist −1 m Building up a face centered cubic lattice No edit summary
- 19:1719:17, 19 March 2007 diff hist +793 Nm Building up a face centered cubic lattice New page: * Consider: # a Cubic Simulation box of length <math>\left. L \right. </math> # a number of lattice positions, <math> \left. M \right. </math> given by: : <math> \left. M = 4 m^3 \ri...
- 19:0719:07, 19 March 2007 diff hist +42 m Lattice Structures No edit summary
- 18:5818:58, 19 March 2007 diff hist +637 Nm Building up a body centered cubic lattice New page: * Consider: # a Cubic Simulation box of length <math>\left. L \right. </math> # a number of lattice positions, <math> \left. M \right. </math> given by: : <math> \left. M = 2 m^3 \ri...
- 18:4818:48, 19 March 2007 diff hist +482 m Building up a simple cubic lattice No edit summary
- 18:3618:36, 19 March 2007 diff hist +90 Nm Building up a simple cubic lattice New page: * Using a Cubic Simulation box of length <math>\left. L \right. </math> [EN CONSTRUCCION]
- 18:3418:34, 19 March 2007 diff hist +177 m Lattice Structures No edit summary
- 18:2918:29, 19 March 2007 diff hist +276 Nm Lattice Structures New page: We will describe some ordered structures that are used as starting configurations in computer simulation of condensed matter. * 2-dimensional systems Square lattice * 3-dimensional...
- 18:2418:24, 19 March 2007 diff hist +187 m Metropolis Monte Carlo →Boundary Conditions
- 18:2118:21, 19 March 2007 diff hist −27 m Metropolis Monte Carlo →Initial configuration
- 18:2018:20, 19 March 2007 diff hist +29 m Metropolis Monte Carlo →Importance sampling
- 18:1518:15, 19 March 2007 diff hist 0 m Ramp model No edit summary
6 March 2007
- 13:0813:08, 6 March 2007 diff hist +118 m Semi-grand ensembles →Fixed pressure and temperature: Semi-grand ensemble: Partition function
5 March 2007
- 17:1317:13, 5 March 2007 diff hist +2 m Semi-grand ensembles →Semi-grand ensemble at fixed volume and temperature
- 17:0517:05, 5 March 2007 diff hist +77 m Semi-grand ensembles →Fixed pressure and temperature: Semigrand ensemble
2 March 2007
- 18:0718:07, 2 March 2007 diff hist +163 m Gibbs-Duhem integration →Example: phase equilibria of one-component system
- 17:1717:17, 2 March 2007 diff hist +62 m Gibbs-Duhem integration →Example: phase equilibria of one-component system
- 17:1617:16, 2 March 2007 diff hist +134 m Gibbs-Duhem integration →Example: phase equilibria of one-component system
- 17:1217:12, 2 March 2007 diff hist +1 m Gibbs-Duhem integration →Peculiarities of the method (Warnings)
- 17:1117:11, 2 March 2007 diff hist +1 m Gibbs-Duhem integration →Peculiarities of the method (Warnings)
- 17:1017:10, 2 March 2007 diff hist +11 m Gibbs-Duhem integration →Peculiarities of the method
- 17:1017:10, 2 March 2007 diff hist +255 m Gibbs-Duhem integration →Peculiarities of the method
- 17:0617:06, 2 March 2007 diff hist +35 m Gibbs-Duhem integration →Example: phase equilibria of one-component system
- 16:4816:48, 2 March 2007 diff hist +392 m Gibbs-Duhem integration →Example: phase equilibria of one-component system
- 16:4216:42, 2 March 2007 diff hist +265 m Gibbs-Duhem integration →Example: phase equilibria of one-compoment system
- 16:1816:18, 2 March 2007 diff hist +172 m Gibbs-Duhem integration →Example: phase equilibria of one-compoment system
- 16:1516:15, 2 March 2007 diff hist +885 m Gibbs-Duhem integration →Example: phase equilibria of one-compoment system
- 13:2413:24, 2 March 2007 diff hist +281 m Gibbs-Duhem integration →Example: phase equilibria of one-compoment system
- 13:1813:18, 2 March 2007 diff hist +77 m Gibbs-Duhem integration →Example: phase equilibria of one-compoment system
- 13:1613:16, 2 March 2007 diff hist −17 m Gibbs-Duhem integration →Basic Features
- 13:1413:14, 2 March 2007 diff hist +275 m Gibbs-Duhem integration →Example: phase equilibria of one-compoment system
- 12:5912:59, 2 March 2007 diff hist −1 m Gibbs-Duhem integration →Example: phase equilibria of one-compoment system
- 12:5912:59, 2 March 2007 diff hist +431 m Gibbs-Duhem integration →Example: phase equilibria of one-compoment system
- 12:4212:42, 2 March 2007 diff hist +144 m Gibbs-Duhem integration →Example: phase equilibria of one-compoment system
- 12:4012:40, 2 March 2007 diff hist +171 m Gibbs-Duhem integration →Basic Features
- 12:3412:34, 2 March 2007 diff hist +4 m Gibbs-Duhem integration →Basic Features
- 12:2812:28, 2 March 2007 diff hist +761 m Gibbs-Duhem integration No edit summary
- 12:1612:16, 2 March 2007 diff hist +486 m Gibbs-Duhem integration No edit summary
- 12:0012:00, 2 March 2007 diff hist +183 Nm Gibbs-Duhem integration New page: The so-called Gibbs-Duhem Integration referes to a number of methods that couple molecular simulation techniques with thermodynamic equations in order to draw phase coexistence lines.
- 11:5511:55, 2 March 2007 diff hist +92 m Monte Carlo in the microcanonical ensemble No edit summary
- 11:4411:44, 2 March 2007 diff hist −6 m Monte Carlo in the microcanonical ensemble No edit summary
- 11:4411:44, 2 March 2007 diff hist +194 m Monte Carlo in the microcanonical ensemble No edit summary
28 February 2007
- 18:1918:19, 28 February 2007 diff hist +3 m Monte Carlo in the microcanonical ensemble →Integration of the kinetic degrees of freedom
- 17:5517:55, 28 February 2007 diff hist +94 m Monte Carlo in the microcanonical ensemble →Integration of the kinetic degrees of freedom
- 17:5317:53, 28 February 2007 diff hist +33 m Monte Carlo in the microcanonical ensemble →Integration of the kinetic degrees of freedom
- 17:5217:52, 28 February 2007 diff hist −85 m Monte Carlo in the microcanonical ensemble →References
- 17:5117:51, 28 February 2007 diff hist −34 m Monte Carlo in the microcanonical ensemble →References
- 17:5117:51, 28 February 2007 diff hist +219 m Monte Carlo in the microcanonical ensemble →References
- 17:4517:45, 28 February 2007 diff hist +72 m Monte Carlo in the microcanonical ensemble →Integration of the kinetic degrees of freedom
- 17:3717:37, 28 February 2007 diff hist +728 m Monte Carlo in the microcanonical ensemble →Integration of the kinetic degrees of freedom
- 16:5416:54, 28 February 2007 diff hist +501 m Monte Carlo in the microcanonical ensemble →Integration of the kinetic degrees of freedom
- 16:3016:30, 28 February 2007 diff hist +52 Nm Monte Carlo in the microcanonical ensemble New page: == Integration of the kinetic degrees of freedom ==
- 16:3016:30, 28 February 2007 diff hist +52 m Metropolis Monte Carlo →Temperature
- 16:2016:20, 28 February 2007 diff hist +51 m Grand canonical ensemble No edit summary
- 16:1316:13, 28 February 2007 diff hist +91 m Grand canonical ensemble →Partition Function
- 16:1016:10, 28 February 2007 diff hist +31 m Grand canonical ensemble No edit summary
- 16:1016:10, 28 February 2007 diff hist +59 m Grand canonical ensemble →Partition Function
- 16:0616:06, 28 February 2007 diff hist +1,182 Nm Grand canonical ensemble New page: == Ensemble variables == * Chemical Potential, <math> \left. \mu \right. </math> * Volume, <math> V </math> * Temperature, <math> T </math> == Partition Function == ''Classical'' Pa...
27 February 2007
- 20:2720:27, 27 February 2007 diff hist +9 m Hard sphere model →References
- 20:2720:27, 27 February 2007 diff hist +23 m Hard sphere model →References
- 19:5519:55, 27 February 2007 diff hist 0 m Hard sphere model →Equations of state
- 19:5519:55, 27 February 2007 diff hist +140 m Hard sphere model →References
- 19:5119:51, 27 February 2007 diff hist +12 m Hard sphere model →Equations of state
- 19:5019:50, 27 February 2007 diff hist +59 m Hard sphere model No edit summary
- 13:1413:14, 27 February 2007 diff hist +1 m 1-dimensional hard rods →Equation of state
- 13:1113:11, 27 February 2007 diff hist −6 m 1-dimensional hard rods →Equation of state
- 13:1113:11, 27 February 2007 diff hist −1 m 1-dimensional hard rods →Equation of state
- 13:1013:10, 27 February 2007 diff hist +218 m 1-dimensional hard rods →Equation of state
- 13:0013:00, 27 February 2007 diff hist +230 m 1-dimensional hard rods →Thermodynamics
- 12:5512:55, 27 February 2007 diff hist +135 m 1-dimensional hard rods →Thermodynamics
- 12:5012:50, 27 February 2007 diff hist +16 m 1-dimensional hard rods →Canonical Ensemble: Configuration Integral
- 12:4712:47, 27 February 2007 diff hist +4 m 1-dimensional hard rods →Thermodynamics
- 12:4712:47, 27 February 2007 diff hist +248 m 1-dimensional hard rods →Canonical Ensemble: Configuration Integral
- 12:3212:32, 27 February 2007 diff hist +62 m Microcanonical ensemble →Thermodynamics
- 12:3012:30, 27 February 2007 diff hist +137 m Microcanonical ensemble →Partition function
- 12:2612:26, 27 February 2007 diff hist −2 m Microcanonical ensemble →Ensemble variables
- 12:2612:26, 27 February 2007 diff hist 0 m Microcanonical ensemble →References
- 12:2512:25, 27 February 2007 diff hist +536 m Microcanonical ensemble No edit summary
- 12:1512:15, 27 February 2007 diff hist +487 Nm Microcanonical ensemble New page: Microcanonical Ensemble (Clasical statistics): Ensemble variables (One component system, 3-dimensional system, ... ): * <math> \left. N \right. </math>: Number of Particles * <math> \le...
- 12:0312:03, 27 February 2007 diff hist +62 m Isothermal-isobaric ensemble No edit summary
26 February 2007
- 17:2717:27, 26 February 2007 diff hist +47 m 1-dimensional hard rods →Canonical Ensemble: Configuration Integral
- 17:2717:27, 26 February 2007 diff hist +1,781 m 1-dimensional hard rods →Canonical Ensemble: Configuration Integral
- 16:4216:42, 26 February 2007 diff hist +49 m 1-dimensional hard rods No edit summary
- 14:5314:53, 26 February 2007 diff hist −33 m Metropolis Monte Carlo →Configuration
- 11:2211:22, 26 February 2007 diff hist +2 m Isothermal-isobaric ensemble No edit summary
- 11:2111:21, 26 February 2007 diff hist +141 m Isothermal-isobaric ensemble No edit summary
23 February 2007
- 21:0621:06, 23 February 2007 diff hist +161 m Isothermal-isobaric ensemble correction of some mistakes
- 20:5020:50, 23 February 2007 diff hist +546 m Metropolis Monte Carlo →Importance sampling
- 20:3520:35, 23 February 2007 diff hist +1,204 m Metropolis Monte Carlo →Importance sampling
- 19:3819:38, 23 February 2007 diff hist +95 m Metropolis Monte Carlo →Main features
- 19:2419:24, 23 February 2007 diff hist +127 m Metropolis Monte Carlo →Configuration
- 19:1319:13, 23 February 2007 diff hist −1 m Metropolis Monte Carlo →Configuration
- 19:0519:05, 23 February 2007 diff hist +2 m Metropolis Monte Carlo →Configuration
- 19:0519:05, 23 February 2007 diff hist +1 m Metropolis Monte Carlo →Main features
- 19:0519:05, 23 February 2007 diff hist +1 m Metropolis Monte Carlo →Configuration
- 19:0419:04, 23 February 2007 diff hist +369 m Metropolis Monte Carlo →Configuration
- 18:5618:56, 23 February 2007 diff hist +205 m Metropolis Monte Carlo →Configuration
- 18:4618:46, 23 February 2007 diff hist +285 m Metropolis Monte Carlo →Main features
- 18:3218:32, 23 February 2007 diff hist +27 m Metropolis Monte Carlo →Main features
- 18:1718:17, 23 February 2007 diff hist −1 m Metropolis Monte Carlo →Main features
- 18:1618:16, 23 February 2007 diff hist +68 m Metropolis Monte Carlo No edit summary
- 17:1617:16, 23 February 2007 diff hist +3 m Talk:CPMD No edit summary current
- 17:1617:16, 23 February 2007 diff hist +174 m Talk:CPMD No edit summary
- 17:0817:08, 23 February 2007 diff hist −2 m Talk:CPMD No edit summary
- 17:0817:08, 23 February 2007 diff hist +49 m Talk:CPMD No edit summary
- 17:0717:07, 23 February 2007 diff hist +164 Nm Talk:CPMD New page: Parallelized? why? I do not like this definition... It is, somehow, a way of coupling DFT calculation with MD simulation --~~~~
- 17:0317:03, 23 February 2007 diff hist +16 m Virial coefficients of model systems No edit summary
- 14:0314:03, 23 February 2007 diff hist +20 m 1-dimensional Ising model No edit summary
- 13:5713:57, 23 February 2007 diff hist −2 m 1-dimensional Ising model No edit summary
- 13:4613:46, 23 February 2007 diff hist +3 m 1-dimensional Ising model minor (I guess) misspellings
- 13:4413:44, 23 February 2007 diff hist +65 m 1-dimensional Ising model No edit summary
- 13:3813:38, 23 February 2007 diff hist +785 m 1-dimensional Ising model No edit summary
- 12:3012:30, 23 February 2007 diff hist 0 m Virial coefficients of model systems misspelling
- 12:2212:22, 23 February 2007 diff hist +31 m 1-dimensional Ising model No edit summary
- 12:2012:20, 23 February 2007 diff hist +62 m Ising model No edit summary
- 12:1912:19, 23 February 2007 diff hist +492 Nm 1-dimensional Ising model New page: Model: Consider a system with <math> N </math> spins in a row. The energy of the system will be given by <math> U = -K \sum_{i=1}^{N-1} S_{i} S_{i+1} </math>, where each variable <mat...
- 11:5111:51, 23 February 2007 diff hist +233 Nm Talk:Ideal gas partition function New page: In the current text it is not clear the separataion between "ideal" and "excess". I think that the ideal part is not just the "kinetic" part (momenta.), the term V**N must also be included...
- 11:3711:37, 23 February 2007 diff hist 0 m Ideal gas partition function Hamiltonian now denoted as H (capital), to avoid confusion with h (Plank's constants)
22 February 2007
- 19:4419:44, 22 February 2007 diff hist +39 m Talk:Ideal gas assumptions No edit summary
- 19:4019:40, 22 February 2007 diff hist +23 m Talk:Ideal gas assumptions No edit summary
- 19:3019:30, 22 February 2007 diff hist +6 m Talk:Ideal gas assumptions No edit summary
- 19:3019:30, 22 February 2007 diff hist +59 Nm Talk:Ideal gas assumptions New page: If the particles have no finite size, are there collisions?
- 19:1019:10, 22 February 2007 diff hist +29 Nm Talk:Second law of thermodynamics New page: Please define variables (Noe)
- 19:0119:01, 22 February 2007 diff hist +728 m Ising model No edit summary
- 17:5417:54, 22 February 2007 diff hist +32 m Hard sphere model →Related systems
- 17:4717:47, 22 February 2007 diff hist +31 m Hard sphere model →Data
- 17:4617:46, 22 February 2007 diff hist 0 m Hard sphere model →Data
- 17:4517:45, 22 February 2007 diff hist 0 m Hard sphere model →Data
- 17:4417:44, 22 February 2007 diff hist +6 m Hard sphere model →Data
- 17:4317:43, 22 February 2007 diff hist +67 m Hard sphere model No edit summary
- 17:4117:41, 22 February 2007 diff hist +11 m Hard sphere model →Related systems
- 17:4017:40, 22 February 2007 diff hist +23 m Hard sphere: virial coefficients No edit summary
- 17:3817:38, 22 February 2007 diff hist +8 m Hard sphere: virial coefficients No edit summary
- 17:3717:37, 22 February 2007 diff hist +56 m Virial coefficients of model systems →Systems
- 17:3517:35, 22 February 2007 diff hist 0 m Hard sphere: virial coefficients HS Virial moved to Hard sphere: virial equation of state: Clarity
- 17:3417:34, 22 February 2007 diff hist −1 m Hard sphere: virial coefficients →References
- 17:3317:33, 22 February 2007 diff hist +237 Nm Hard sphere: virial coefficients New page: Virial Coefficients of Hard Spheres and Hard Disks See Ref 1. == References == #Stanislav Labík, Jirí Kolafa, and Anatol Malijevský, Virial coefficients of hard spheres and hard disk...
- 17:3117:31, 22 February 2007 diff hist +70 m Virial coefficients of model systems No edit summary
- 17:2417:24, 22 February 2007 diff hist +20 m Models No edit summary
- 17:2017:20, 22 February 2007 diff hist +9 m Widom-Rowlinson model No edit summary
- 17:1817:18, 22 February 2007 diff hist +4 m Widom-Rowlinson model No edit summary
- 17:1817:18, 22 February 2007 diff hist +1 m Widom-Rowlinson model →References
- 17:1717:17, 22 February 2007 diff hist +2 m Widom-Rowlinson model →References
- 17:1717:17, 22 February 2007 diff hist +121 m Widom-Rowlinson model →References
- 17:1317:13, 22 February 2007 diff hist +18 m Widom-Rowlinson model No edit summary
- 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