Surface tension: Difference between revisions
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== Thermodynamics == | == Thermodynamics == | ||
In the [[Canonical ensemble]]: | In the [[Canonical ensemble]] the surface tension is formally given as: | ||
:<math> \gamma = \frac{ \partial A (N,V,T, {\mathcal A} )}{\partial {\mathcal A} } </math>; | :<math> \gamma = \frac{ \partial A (N,V,T, {\mathcal A} )}{\partial {\mathcal A} } </math>; | ||
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*<math> {\mathcal A} </math> is the surface area | *<math> {\mathcal A} </math> is the surface area | ||
*<math>A</math> is the [[Helmholtz energy function]] | *<math>A</math> is the [[Helmholtz energy function]] | ||
==Computer Simulation== | ==Computer Simulation== | ||
Revision as of 11:09, 1 August 2007
The surface tension, , is a measure of the work required to create a surface.
Thermodynamics
In the Canonical ensemble the surface tension is formally given as:
- ;
where
- is the number of particles
- is the volume
- is the temperature
- is the surface area
- is the Helmholtz energy function
Computer Simulation
A review on different techniques to compute surface (interface) tension can be found in the paper by Gloor et al.
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:
The calculation is usually carried out using Monte Carlo simulation
If liquid-vapour equilibrium occurs, the plot of the chemical potential, , as a function of shows a loop.
Using basic thermodynamic procedures (Maxwell construction) it is possible to compute the densities of the two phases;