User contributions for Carl McBride
A user with 9,509 edits. Account created on 15 February 2007.
29 January 2008
- 16:3216:32, 29 January 2008 diff hist +4 m Thermodynamic relations Added internal link
- 16:3016:30, 29 January 2008 diff hist +28 m Thermodynamic integration No edit summary
- 16:2316:23, 29 January 2008 diff hist +114 m Thermal expansion coefficient Defined variables
- 16:2116:21, 29 January 2008 diff hist +147 m Maxwell's relations Defined variables
- 16:1716:17, 29 January 2008 diff hist +5 m Heat capacity →At constant volume: Added internal link
- 16:1716:17, 29 January 2008 diff hist +4 m Gibbs energy function Added internal link current
- 16:0916:09, 29 January 2008 diff hist +8 m Gay-Lussac's law Added internal link
- 16:0916:09, 29 January 2008 diff hist +92 m First law of thermodynamics No edit summary
- 16:0616:06, 29 January 2008 diff hist +4 m Compressibility Added internal link
- 16:0516:05, 29 January 2008 diff hist +7 m Chemical potential →Classical thermodynamics: Added internal links
- 16:0416:04, 29 January 2008 diff hist +4 m Charles's law Added internal link
- 16:0316:03, 29 January 2008 diff hist +4 m Boyle's law Added internal link
- 15:5615:56, 29 January 2008 diff hist +1 m Combining rules →Admur and Mason: Corrected Ref. number.
- 15:1915:19, 29 January 2008 diff hist +119 m Enthalpy No edit summary
- 14:2414:24, 29 January 2008 diff hist +636 N Langevin equations New page: {{stub-general}} The generalised '''Langevin equation''' can be considered as a mathematical rearrangement of the Liouville's theorem. :<math>\frac{da(t)}{dt}= i\Omega a(t) - \int_0^... current
- 14:0814:08, 29 January 2008 diff hist +1 m Non-equilibrium thermodynamics No edit summary
- 11:5111:51, 29 January 2008 diff hist +174 m Wikis and Science 2.0 No edit summary
28 January 2008
- 16:0016:00, 28 January 2008 diff hist −8 m Ornstein-Zernike relation from the grand canonical distribution function No edit summary
- 12:1712:17, 28 January 2008 diff hist +2 m Liquid crystals →Phases: Spelling error
- 12:0712:07, 28 January 2008 diff hist +1,055 N Odd-even effect New page: {{stub-general}} ==References== #[http://dx.doi.org/10.1063/1.1681578 S. Marcelja "Chain ordering in liquid crystals. I. Even-odd effect", Journal of Chemical Physics '''60''' pp. 3599- (... current
- 11:4111:41, 28 January 2008 diff hist +33 m Liquid crystals No edit summary
- 11:3611:36, 28 January 2008 diff hist +206 m Liquid crystals →Models
- 11:3111:31, 28 January 2008 diff hist +266 N Single site anisotropic soft-core potential New page: {{Stub-general}} ==References== #[http://dx.doi.org/10.1063/1.2825292 Juho S. Lintuvuori and Mark R. Wilson "A new anisotropic soft-core model for the simulation of liquid crystal mesophas...
- 11:2911:29, 28 January 2008 diff hist +49 Idealised models →'Soft' models
25 January 2008
- 15:4415:44, 25 January 2008 diff hist −50 m Grand canonical Monte Carlo Removed (redundant) first line.
- 14:2214:22, 25 January 2008 diff hist +102 m Grand canonical Monte Carlo Removed stub template
- 14:1314:13, 25 January 2008 diff hist +75 m Grand canonical Monte Carlo →Theoretical basis: Slight tidy.
- 12:4012:40, 25 January 2008 diff hist +72 m Grand canonical Monte Carlo Slight tidy.
- 12:0812:08, 25 January 2008 diff hist +1,732 User talk:Carl McBride No edit summary
24 January 2008
- 13:3813:38, 24 January 2008 diff hist +163 m Statistical mechanics →General interest
- 12:0712:07, 24 January 2008 diff hist +58 m Idealised models No edit summary
- 11:1811:18, 24 January 2008 diff hist +229 m Stockmayer potential →References
- 11:0011:00, 24 January 2008 diff hist +82 m Researchers and research groups →United States of America
- 10:5810:58, 24 January 2008 diff hist +133 m Conferences →May
23 January 2008
- 18:3418:34, 23 January 2008 diff hist +59 m Stockmayer potential →Critical properties
- 18:3018:30, 23 January 2008 diff hist +218 m Stockmayer potential No edit summary
- 18:2618:26, 23 January 2008 diff hist +71 m Stockmayer potential No edit summary
- 18:2318:23, 23 January 2008 diff hist +1,671 N Stockmayer potential New page: The '''Stockmayer potential''' consists of the Lennard-Jones model with an embedded point dipole. Thus the Stockmayer potential becomes: :<math> \Phi(r, \theta_1, \theta_2, \phi) = 4 ...
- 17:3617:36, 23 January 2008 diff hist +27 Idealised models →'Soft' models
- 17:3617:36, 23 January 2008 diff hist +27 m Idealised models →'Hard' models
- 16:0516:05, 23 January 2008 diff hist +620 m Chiral phases →Helical twisting power
- 15:4015:40, 23 January 2008 diff hist +199 m Nematic phase →Biaxial nematic phase
- 12:5712:57, 23 January 2008 diff hist −18 m Conferences No edit summary
- 11:3011:30, 23 January 2008 diff hist +10 m List of ab initio water models Removed table of contents.
- 11:3011:30, 23 January 2008 diff hist +10 m List of empirical water models Removed table of contents.
- 11:2911:29, 23 January 2008 diff hist +2 m Materials modelling and computer simulation codes Removed table of contents.
- 11:2911:29, 23 January 2008 diff hist +8 m Materials modelling and computer simulation codes Removed table of contents.
- 11:1611:16, 23 January 2008 diff hist −46 m Force fields No edit summary
- 11:0811:08, 23 January 2008 diff hist +478 m Models Added breif descriptions.
- 10:3410:34, 23 January 2008 diff hist +4 m Ideal gas partition function Slight tidy up