Abstract
Interface equations are derived for both binary diffusive and binary fluid systems subjected to nonequilibrium conditions, starting from coarse-grained (mesoscopic) models. The equations are used to describe thermocapillary motion of a droplet in both purely diffusive and fluid cases, and the results are compared with numerical simulations. A mesoscopic chemical potential shift owing to the temperature gradient, and associated mesoscopic corrections involved in droplet motion, are elucidated.
Similar content being viewed by others
References
See, e.g., J. S. Langer, inChance and Matter Les Houches Summer School (eds. J. Souletie, J. Vannimenus and R. Stora, North Holland, N. Y., 1086);Dynamics of Curved Fronts (ed. R. Pelce, Academic, N.Y., 1988); D. Kessler, J. Koplik and H. Levine,Adv. Phys. 37:255 (1988); J. S. Langer and L. Turski,Acta Metall. 25:267 (1977); D. Jasnow and J. Viñals,Phys. Rev. 40:3864 (1989).
K. Kawasaki and T. Ohta,Prog. Theor. Phys. 68:129 (1982);Physica A 118:175 (1983).
H. Lamb,Hydrodynamics, sixth ed. (Dover, N. Y., 1932) Sec. 337.
N. O. Young, J. S. Goldstein, and M. J. Block,J. Fluid. Mech. 6:350–356 (1959).
See, for example, the review article by R. S. Subramanian, inTransport Processes an Bubbles, Drops and Particles, ed. by R. P. Chhabra and D. De Kee, (Hemisphere Pub. Corp., N. Y. 1992).
R. Bhagavatula and D. Jasnow,J. Chem. Phys., July 1996.
P. C. Hohenberg and B. I. Halperin,Rev. Mod. Phys. 49:435 (1977).
D. Jasnow and J. Vinals,Phys. of Fluids 7:747 (1996).
See eg., J. S. Langer, inSolids far from Equilibrium, ed. by C. Godreche (Cambridge 1992).
D. Jasnow,Rep. Prog. Phys. 47:1059–1132 (1984).
S. Fisk and B. Widom,J. Chem. Phys. 50:3219 (1969).
J. R. Rowlinson and B. Widom,Molecular Theory of Capillarity, (Clarendon Press, Oxford 1982).
For a recent review see, A. J. Bray,Adv. in Physics, 1996.
T. Ohta,Ann. Phys. (N.Y.)158:31 (1984).
K. Kitahara, Y. Oono and D. Jasnow,Mod. Phys. Lett. B 2:765 (1988).
J. Llambias and D. Jasnow (unpublished). Also, see J. Llambías, A. Shinozaki and D. Jasnow, NASA Conference Publication 3276, 207 (1994).
H. W. Alt and I. Pawlow,Physica D 59:389–416 (1992).
D. Boyanovsky, D. Jasnow, J. Llambías and F. Takakura,Phys. Rev. E 51:5453 (1995).
R. Bhagavatula, J. Llambías and D. Jasnow, unpublished.
C. Yeung, J. M. Mozos, A. Hernandez-Machado and D. Jasnow,J. Stat. Phys. 70:1149 (1993).
D. Jasnow and J. Viñals,Phys. Rev. A 41:6910 (1990).
S. Sarkar and D. Jasnow,Phys. Rev. A 39:5299 (1989). A numerical method of solving 2d interface equations of this sort is discussed; for example, by J. Viñals and D. Jasnow,Phys. Rev. A 46:7777 (1992).
G. Caginalp,Ann. Phys. (N.Y.)172:136 (1986).
If the droplet were moving steadily as a solid object, the interface velocity would vanish in the CM frame, i.e., the rest frame of the droplet. Then would havev n =V cos(θ) andv t = −V sin(θ).
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Bhagavatula, R., Jasnow, D. & Ohta, T. Nonequilibrium interface equations: An application to thermocapillary motion in binary systems. J Stat Phys 88, 1013–1031 (1997). https://doi.org/10.1007/BF02732424
Received:
Accepted:
Issue Date:
DOI: https://doi.org/10.1007/BF02732424