Communications: Evidence for the role of fluctuations in the thermodynamics of nanoscale drops and the implications in computations of the surface tension.

Test-area deformations are used to analyze vapor-liquid interfaces of Lennard-Jones particles by molecular dynamics simulation. For planar vapor-liquid interfaces the change in free energy is captured by the average of the corresponding change in energy, the leading-order contribution. This is consistent with the commonly used mechanical (pressure-tensor) route for the surface tension. By contrast for liquid drops, one finds a large second-order contribution associated with fluctuations in energy. Both the first- and second-order terms make comparable contributions, invalidating the mechanical relation for the surface tension of small drops. The latter is seen to increase above the planar value for drop radii of approximately 8 particle diameters, followed by an apparent weak maximum and slow decay to the planar limit, consistent with a small negative Tolman length.

[1]  J. Henderson,et al.  The density profile and surface tension of a drop , 1981 .

[2]  K. Gubbins,et al.  A microscopic theory for spherical interfaces: Liquid drops in the canonical ensemble , 1986 .

[3]  B. Widom,et al.  Some Topics in the Theory of Fluids , 1963 .

[4]  A. H. Falls,et al.  Structure and stress in spherical microstructures , 1981 .

[5]  D. Bedeaux,et al.  Derivation of microscopic expressions for the rigidity constants of a simple liquid—vapor interface , 1992 .

[6]  Daan Frenkel,et al.  Computer simulation study of gas–liquid nucleation in a Lennard-Jones system , 1998 .

[7]  D. Oxtoby,et al.  Nonclassical nucleation theory for the gas-liquid transition , 1988 .

[8]  Alan E van Giessen,et al.  Direct determination of the Tolman length from the bulk pressures of liquid drops via molecular dynamics simulations. , 2009, The Journal of chemical physics.

[9]  C. Croxton Fluid interfacial phenomena , 1986 .

[10]  C. Jacolin,et al.  Density profiles and surface tension of spherical interfaces. Numerical results for nitrogen drops and bubbles , 1985 .

[11]  H. Reiss,et al.  Understanding the Limitations of the Virial in the Simulation of Nanosystems: A Puzzle That Stimulated the Search for Understanding† , 2004 .

[12]  A. Shchekin,et al.  Validity of Tolman's equation: How large should a droplet be? , 1998 .

[13]  Hans Hasse,et al.  Comprehensive study of the vapour–liquid coexistence of the truncated and shifted Lennard–Jones fluid including planar and spherical interface properties , 2006 .

[14]  D. Bedeaux,et al.  Pressure tensor of a spherical interface , 1992 .

[15]  K. Binder,et al.  Simulation of vapor-liquid coexistence in finite volumes: a method to compute the surface free energy of droplets. , 2009, Physical review. E, Statistical, nonlinear, and soft matter physics.

[16]  J. Lekner,et al.  Surface tension and energy of a classical liquid-vapour interface , 1977 .

[17]  K. Gubbins,et al.  A molecular dynamics study of liquid drops , 1984 .

[18]  George Jackson,et al.  Test-area simulation method for the direct determination of the interfacial tension of systems with continuous or discontinuous potentials. , 2005, The Journal of chemical physics.

[19]  John S. Rowlinson,et al.  Molecular Theory of Capillarity , 1983 .

[20]  R. Tolman The Effect of Droplet Size on Surface Tension , 1949 .

[21]  J. Henderson,et al.  Statistical mechanics of inhomogeneous fluids , 1982, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[22]  Jianzhong Wu,et al.  Toward a Quantitative Theory of Ultrasmall Liquid Droplets and Vapor-Liquid Nucleation , 2008 .

[23]  X. Zeng,et al.  Heterogeneous nucleation on mesoscopic wettable particles: A hybrid thermodynamic/density-functional theory , 2002 .

[24]  A. F. Bakker,et al.  Molecular dynamics of the surface tension of a drop , 1992 .

[25]  S. Yoo,et al.  The Tolman length: is it positive or negative? , 2005, Journal of the American Chemical Society.

[26]  M. Baus,et al.  Computer simulation study of the local pressure in a spherical liquid–vapor interface , 2000 .

[27]  G. Jackson,et al.  The nature of the calculation of the pressure in molecular simulations of continuous models from volume perturbations. , 2006, The Journal of chemical physics.

[28]  R. Eppenga,et al.  Monte Carlo study of the isotropic and nematic phases of infinitely thin hard platelets , 1984 .