Surface tension: Difference between revisions
Jump to navigation
Jump to search
mNo edit summary |
|||
Line 13: | Line 13: | ||
*<math>A</math> is the [[Helmholtz energy function]] | *<math>A</math> is the [[Helmholtz energy function]] | ||
==Computer Simulation== | ==Computer Simulation== | ||
=== Liquid-Vapour Interfaces of one component systems === | |||
* Binder procedure | * Binder procedure | ||
For given conditions of volume and temperature, the Helmholtz energy function is computed as a function of the number of molecules: | |||
<math> A(N;V,T) </math> | |||
If liquid-vapour equilibrium occurs, the plot of the chemical potential, <math> \mu \equiv (\partial A/\partial N)_{V,T} </math> | |||
is a function of <math> N </math> shows a loop. | |||
Using basic thermodynamic procedures (Maxwell construction) it is possible | |||
to compute the densities of the two phases; <math> \rho_v, \rho_l </math> | |||
* Explicit interface | * Explicit interface | ||
==References== | ==References== | ||
[[category]] | [[category]] |
Revision as of 10:54, 1 August 2007
The surface tension, , is a measure of the work required to create a surface. In the Canonical ensemble: two phases;
- ;
where
- is the number of particles
- is the volume
- is the temperature
- is the surface area
- is the Helmholtz energy function
Computer Simulation
Liquid-Vapour Interfaces of one component systems
- Binder procedure
For given conditions of volume and temperature, the Helmholtz energy function is computed as a function of the number of molecules:
If liquid-vapour equilibrium occurs, the plot of the chemical potential, is a function of shows a loop.
Using basic thermodynamic procedures (Maxwell construction) it is possible to compute the densities of the two phases;
- Explicit interface