Difference between revisions of "Surface tension"

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==Computer Simulation==
 
==Computer Simulation==
A review of the  different techniques that can be used to compute the surface (interface) tension can be found in the paper by Gloor ''et al.'' (Ref. 1).
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Different techniques may be used to compute this quantity, such as the traditional [[stress | stress tensor]] route or the more recent [[test area method]]. A review can be found in the paper by Gloor ''et al.'' (Ref. 1).
  
 
==Liquid-Vapour Interfaces of one component systems ==
 
==Liquid-Vapour Interfaces of one component systems ==

Revision as of 11:58, 7 February 2008

The surface tension,  \gamma , is a measure of the work required to create an interface between two bulk phases.

Thermodynamics

In the Canonical ensemble the surface tension is formally given as:

 \gamma = \frac{ \partial A (N,V,T, {\mathcal A} )}{\partial  {\mathcal A} } ;

where

Computer Simulation

Different techniques may be used to compute this quantity, such as the traditional stress tensor route or the more recent test area method. A review can be found in the paper by Gloor et al. (Ref. 1).

Liquid-Vapour Interfaces of one component systems

Binder procedure

Here, only an outline of the procedure is presented, more details can be found in Reference 2. For given conditions of volume and temperature, the Helmholtz energy function is computed as a function of the number of molecules,  A(N;V,T). The calculation is usually carried out using Monte Carlo simulation using periodic boundary conditions If liquid-vapour equilibrium occurs, a plot of the chemical potential,  \mu \equiv (\partial A/\partial N)_{V,T} , as a function of  N shows a loop. Using basic thermodynamic procedures (Maxwell's equal area construction) it is possible to compute the densities of the two phases;  \rho_v, \rho_l at liquid-vapour equilibrium. Considering the thermodynamic limit for densities  \rho with  \rho_v < \rho < \rho_l the Helmholtz energy function will be:

 A(N) = - p_{eq} V + \mu_{eq} N + \gamma {\mathcal A}(N)

where the quantities with the subindex "eq" are those corresponding to the fluid-phase equilibrium situation. From the previous equation one can write

 \Omega (N) \equiv A(N)  - \mu_{eq} N = - p_{eq} V + \gamma {\mathcal A}(N)  .

For appropriate values of  N one can estimate the value of the surface area,  {\mathcal A} (See MacDowell et al., Ref. 3), and compute  \gamma directly as:

 \gamma = \frac{ \Omega(N) + p_{eq} V } { {\mathcal A}(N) } = \frac{ \Omega(N) - \frac{1}{2}(\Omega(N_l)+\Omega(N_v)) }{{\mathcal A}(N)}

where  N_l and  N_v are given by:  N_l = V \cdot \rho_l and  N_v = V \cdot \rho_v

Explicit interfaces

In these methods one performs a direct simulation of the two-phase system. Periodic boundary conditions are usually employed. Simulation boxes are elongated in one direction, and the interfaces are built (and expected to stay) perpendicular to such a direction. Taking into account the canonical ensemble definition (see above), one computes the change in the Helmholtz energy function when a small (differential) change of the surface area is performed at constant  V, T, and  N . The explicit equations can be written in terms of the diagonal components of the pressure tensor of the system. Mechanical arguments can also be invoked to arrive at equivalent conclusions (see Ref 1 for a detailed discussion of these issues).

System-size analysis

The system-size dependence of the results for  \gamma have to be taken into account in order to obtain accurate results for model systems. Spurious effects that occur due to small system sizes can appear in the explicit interface methods. (See P.Orea et al. Ref. 4).

Mixtures

Different ensembles can be used to compute the surface tension between two phases in the case of mixtures (See for example see Y. Zhang et al. Ref 5). The simulation techniques are essentially the same as those for one-component systems, but different ensembles can be more adequate. For instance, for binary mixtures (with components 1 and 2), the isothermal-isobaric ensemble,  N_1,N_2,p.T is a more natural ensemble to compute  \gamma using explicit interface techniques (See Ref. 6 as an example). In the case of the Binder technique the analysis can be carried out by fixing the total number of particles:  N \equiv N_1 + N_2 , the pressure,  p , and the temperature  T . Then one will have to compute the variation of the adequate thermodynamic potential as a function of the composition, e.g.  x_1 = N_1/N .

See also

References

  1. Guy J. Gloor, George Jackson, Felipe J. Blas and Enrique de Miguel "Test-area simulation method for the direct determination of the interfacial tension of systems with continuous or discontinuous potentials", Journal of Chemical Physics 123 134703 (2005)
  2. K. Binder "Monte Carlo calculation of the surface tension for two- and three-dimensional lattice-gas models", Physical Review A 25 pp. 1699 - 1709 (1982)
  3. L. G. MacDowell, V. K. Shen, and J. R. Errington "Nucleation and cavitation of spherical, cylindrical, and slablike droplets and bubbles in small systems", Journal of Chemical Physics 125 034705 (2006)
  4. Pedro Orea, Jorge López-Lemus, and José Alejandre, "Oscillatory surface tension due to finite-size effects", Journal of Chemical Physics 123 114702 (6 pages) (2005)
  5. Yuhong Zhang, Scott E. Feller, Bernard R. Brooks, and Richard W. Pastor, "Computer simulation of liquid/liquid interfaces. I. Theory and application to octane/water", Journal of Chemical Physics, 103, pp. 10252-10266 (1995)
  6. E. de Miguel, N. G. Almarza, and G. Jackson, "Surface tension of the Widom-Rowlinson model", Journal of Chemical Physics, 127, 034707 (10 pages) (2007)
  7. John G. Kirkwood and Frank P. Buff "The Statistical Mechanical Theory of Surface Tension", Journal of Chemical Physics 17 pp. 338-343 (1949)
  8. Charles H. Bennett "Efficient estimation of free energy differences from Monte Carlo data", Journal of Computational Physics 22 pp. 245-268 (1976)
  9. J. Miyazaki, J. A. Barker and G. M. Pound "A new Monte Carlo method for calculating surface tension", Journal of Chemical Physics 64 pp. 3364-3369 (1976)