User contributions for 161.111.27.7
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20 August 2008
- 14:4614:46, 20 August 2008 diff hist +144 N Talk:Hard square lattice model New page: Should it be hard square model the title of this page? where are the lattices? --~~~~
8 July 2008
- 10:4010:40, 8 July 2008 diff hist +167 Wang-Landau method some additions
5 September 2007
- 09:2209:22, 5 September 2007 diff hist +349 Cluster algorithms →Probability-Changing Cluster Algorithm
9 August 2007
- 10:0510:05, 9 August 2007 diff hist +37 N Talk:Diffusion New page: hay que revisar las definiciones ---- current
31 July 2007
- 18:4118:41, 31 July 2007 diff hist +113 Surface tension No edit summary
5 July 2007
- 14:0314:03, 5 July 2007 diff hist −5 Ramp model No edit summary
- 14:0214:02, 5 July 2007 diff hist +5 Ramp model No edit summary
11 June 2007
- 11:4711:47, 11 June 2007 diff hist −1 Inverse Monte Carlo →References
- 11:4511:45, 11 June 2007 diff hist +207 Inverse Monte Carlo →References
8 June 2007
- 18:3518:35, 8 June 2007 diff hist −2 Inverse Monte Carlo No edit summary
- 18:3418:34, 8 June 2007 diff hist +26 Configuration analysis No edit summary
- 18:0518:05, 8 June 2007 diff hist +27 Inverse Monte Carlo No edit summary
- 18:0418:04, 8 June 2007 diff hist 0 Inverse Monte Carlo No edit summary
- 18:0418:04, 8 June 2007 diff hist +258 N Inverse Monte Carlo New page: Inverse Monte Carlo refers to the numerical techniques to solve the so-called inverse problem in fluids. i.e. Given the structural information (distribution functions) the inverse Monte Ca...
- 18:0118:01, 8 June 2007 diff hist +25 Monte Carlo methods No edit summary
- 17:5917:59, 8 June 2007 diff hist +18 N Configuration analysis New page: *Voronoi cells
- 17:5817:58, 8 June 2007 diff hist +28 Computer simulation techniques No edit summary
23 March 2007
- 12:1212:12, 23 March 2007 diff hist +42 Lennard-Jones model No edit summary
- 12:1112:11, 23 March 2007 diff hist +33 Lennard-Jones model →Features
- 12:1012:10, 23 March 2007 diff hist +195 Lennard-Jones model →Features
- 12:0612:06, 23 March 2007 diff hist +16 Lennard-Jones model →Argon
21 March 2007
- 14:1414:14, 21 March 2007 diff hist +115 N Talk:Hard sphere: virial coefficients New page: References for dimension > 3 are required (I guess) --~~~~
20 March 2007
- 11:4511:45, 20 March 2007 diff hist +3 Building up a face centered cubic lattice No edit summary
19 March 2007
- 17:1117:11, 19 March 2007 diff hist +82 N Talk:Hard sphere model New page: Please define CDOT --~~~~
6 March 2007
- 12:0312:03, 6 March 2007 diff hist +41 Semi-grand ensembles →Fixed pressure and temperature: Semi-grand ensemble: Partition function
- 11:2811:28, 6 March 2007 diff hist +156 Semi-grand ensembles →Fixed pressure and temperature: Semi-grand ensemble: Partition function
- 11:2411:24, 6 March 2007 diff hist −4 Semi-grand ensembles →Semi-grand ensemble at fixed volume and temperature: elliminated the link in thermodynamic potential (everything is a thermodinamic pot.)
5 March 2007
- 16:0316:03, 5 March 2007 diff hist +27 Semi-grand ensembles →Fixed pressure and temperature: Semigrand esemble
- 16:0216:02, 5 March 2007 diff hist +21 Semi-grand ensembles →Fixed pressure and temperature: Semigrand esemble
- 16:0016:00, 5 March 2007 diff hist +507 Semi-grand ensembles →Fixed pressure and temperature
- 15:5215:52, 5 March 2007 diff hist +1 Semi-grand ensembles →General Features
- 15:5215:52, 5 March 2007 diff hist +119 Semi-grand ensembles →Semi-grand ensemble at fixed volume and temperature
- 15:4615:46, 5 March 2007 diff hist +20 Semi-grand ensembles →Semi-grand ensemble at fixed volume and temperature
- 15:4315:43, 5 March 2007 diff hist +13 Semi-grand ensembles →Canonical Ensemble: fixed volume, temperature and number(s) of molecules
- 15:4215:42, 5 March 2007 diff hist +56 Semi-grand ensembles →Fixed pressure and temperature
- 15:3915:39, 5 March 2007 diff hist +231 Semi-grand ensembles →Semi-grand ensemble at fixed volume and temperature
- 15:3515:35, 5 March 2007 diff hist +163 Semi-grand ensembles →Semi-grand ensemble at fixed volume and temperature
- 14:0314:03, 5 March 2007 diff hist +266 Semi-grand ensembles →Semi-grand ensemble at fixed volume and temperature
- 13:1413:14, 5 March 2007 diff hist +214 Semi-grand ensembles →Semi-grand ensemble at fixed volume and temperature
- 13:0913:09, 5 March 2007 diff hist +104 Semi-grand ensembles No edit summary
- 13:0813:08, 5 March 2007 diff hist +426 Semi-grand ensembles →Semi-grand ensemble at fixed volume and temperature
- 13:0013:00, 5 March 2007 diff hist +700 Semi-grand ensembles →Fixed Volume and Temperature
- 12:4712:47, 5 March 2007 diff hist +286 N Semi-grand ensembles New page: == General Features == Semi-grand ensembles are used in Monte Carlo simulation of mixtures. In this ensembles the total number of molecules is fixed, but the composition can change. == F...
28 February 2007
- 14:5914:59, 28 February 2007 diff hist 0 Microcanonical ensemble →Partition function: N instead of n
27 February 2007
26 February 2007
- 10:1910:19, 26 February 2007 diff hist +74 Isothermal-isobaric ensemble No edit summary
23 February 2007
- 10:1310:13, 23 February 2007 diff hist +102 Talk:Ideal gas assumptions No edit summary current
22 February 2007
- 11:0911:09, 22 February 2007 diff hist +440 Flexible molecules No edit summary
- 10:5810:58, 22 February 2007 diff hist +225 N Flexible molecules New page: Modelling of internal degrees of freedom, usual techniques: == Bond distances == * Atoms linked by a chemical bond (stretching): <math> V_{str} (r_{12}) = \frac{1}{2} K_{str} ( r_{12} -...
- 10:4910:49, 22 February 2007 diff hist +43 Models No edit summary
21 February 2007
- 17:4617:46, 21 February 2007 diff hist +2 Equation of State: Ideal Gas No edit summary
- 17:4317:43, 21 February 2007 diff hist +1 Ideal gas No edit summary
- 17:4317:43, 21 February 2007 diff hist +50 Ideal gas No edit summary
- 17:4117:41, 21 February 2007 diff hist +518 N Equation of State: Ideal Gas New page: The Ideal Gas Equation of State is given by: * <math> \left. p V = N k_B T \right. </math> * <math> \left. p V = n R T \right.</math> where: * <math> p </math> is the pressure * <math>...
20 February 2007
- 10:4210:42, 20 February 2007 diff hist −1 Canonical ensemble →Free energy and Partition Function
- 10:4210:42, 20 February 2007 diff hist +6 Canonical ensemble →Free energy and Partition Function
19 February 2007
- 12:1412:14, 19 February 2007 diff hist +672 N Hard core Yukawa potential New page: Hard Core Yukawa Potential (Attractive): <math> V\left( r \right) = \left\{ \begin{array}{ccc} \infty & ; & r < \sigma \\ - \left( \frac{ \epsilon \sigma }{r}\right) \exp \left[- \kappa...
16 February 2007
- 10:1110:11, 16 February 2007 diff hist 0 Hard sphere model No edit summary
- 10:1110:11, 16 February 2007 diff hist +219 N Hard sphere model New page: The hard sphere interaction potential is givne by V(r) = \infinity if r < sigma; and V(r) = 0; if r > sigma. where V(r) is the potential energy between two spheres at a distance r, an...