Nonpotential Effects in Nonlinear Dynamics of Marangoni convection
暂无分享,去创建一个
Alexander A. Nepomnyashchy | L. M. Pismen | Alexander A. Golovin | L. Pismen | A. Nepomnyashchy | A. Golovin
[1] A. Nepomnyashchy,et al. Combined action of different mechanisms of convective instability in multilayer systems. , 1999, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.
[2] Michael Bestehorn,et al. Square cells in surface-tension-driven Bénard convection: experiment and theory , 1998, Journal of Fluid Mechanics.
[3] Schatz,et al. Onset of Surface-Tension-Driven Bénard Convection. , 1995, Physical review letters.
[4] Hermann Riecke,et al. Instabilities and spatio-temporal chaos in hexagon patterns with rotation , 1998, patt-sol/9810006.
[5] Jean Bragard,et al. Bénard–Marangoni convection: planforms and related theoretical predictions , 1998, Journal of Fluid Mechanics.
[6] L. Pismen,et al. Pattern formation in large-scale Marangoni convection with deformable interface , 1995 .
[7] Schatz,et al. Long-wavelength instability in surface-tension-driven Bénard convection. , 1995, Physical review letters.
[8] L. Pismen,et al. New amplitude equation for Boussinesq convection and nonequilateral hexagonal patterns , 1995 .
[9] P. Colinet,et al. Bénard-Marangoni convection of a binary mixture as an example of an oscillatory bifurcation under strong symmetry-breaking effects , 2000 .
[10] Alexander A. Nepomnyashchy,et al. Interfacial Phenomena and Convection , 2001 .
[11] L. Pismen,et al. Interaction between short‐scale Marangoni convection and long‐scale deformational instability , 1994 .
[12] Bestehorn. Phase and amplitude instabilities for Bénard-Marangoni convection in fluid layers with large aspect ratio. , 1993, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.
[13] Edgar Knobloch,et al. Pattern selection in long-wavelength convection , 1990 .
[14] L. Pismen,et al. Nonlinear evolution and secondary instabilities of Marangoni convection in a liquid–gas system with deformable interface , 1997, Journal of Fluid Mechanics.
[15] Haim H. Bau,et al. Control of Marangoni–Bénard convection , 1999 .
[16] Steinberg,et al. Observation of coexisting upflow and downflow hexagons in Boussinesq Rayleigh-Bénard convection. , 1996, Physical review letters.
[17] L. Pismen,et al. Stability of rolls and hexagonal patterns in non-potential systems , 2000 .
[18] Ashutosh Sharma,et al. Pattern formation in unstable thin liquid films under the influence of antagonistic short- and long-range forces , 1999 .
[19] Mean flow in hexagonal convection: stability and nonlinear dynamics , 2001, physics/0107058.
[20] H. Brand. Envelope Equations Near the Onset of a Hexagonal Pattern : Complex Dynamics in Nonlinear Systems , 1989 .
[21] A. Thess,et al. Direct numerical simulation of Marangoni convection in a two-fluid system , 1999 .
[22] Robert E. Kelly,et al. Feedback control of weakly nonlinear Rayleigh–Bénard–Marangoni convection , 2001, Journal of Fluid Mechanics.
[23] Manuel G. Velarde,et al. Convective instability: A physicist's approach , 1977 .
[24] Michael F. Schatz,et al. Long-wavelength surface-tension-driven Bénard convection: experiment and theory , 1997, Journal of Fluid Mechanics.
[25] P. Umbanhowar,et al. Hexagons, kinks, and disorder in oscillated granular layers. , 1995, Physical review letters.
[26] M. Velarde,et al. Onset of oscillatory interfacial instability and wave motions in Bénard layers , 2001 .
[27] Phase instabilities in hexagonal patterns , 1998, patt-sol/9805007.
[28] Modulated two-dimensional patterns in reaction–diffusion systems , 1999, European Journal of Applied Mathematics.
[29] S. Bankoff,et al. Long-scale evolution of thin liquid films , 1997 .
[30] Hirofumi Tomita,et al. Numerical simulation of pattern formation in the Bénard–Marangoni convection , 2000 .
[31] Alexander Oron,et al. Nonlinear dynamics of three-dimensional long-wave Marangoni instability in thin liquid films , 2000 .
[32] Thess,et al. Planform selection in Bénard-Marangoni convection: l hexagons versus g hexagons. , 1995, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.
[33] H. Swinney,et al. Transition from a uniform state to hexagonal and striped Turing patterns , 1991, Nature.
[34] Steven A. Orszag,et al. Surface-tension-driven Bénard convention at infinite Prandtl number , 1995, Journal of Fluid Mechanics.
[35] G. Sivashinsky,et al. Hexagonal structure of large-scale Marangoni convection , 1991 .
[36] Manuel G. Velarde,et al. Drops, liquid layers and the Marangoni effect , 1998, Philosophical Transactions of the Royal Society of London. Series A: Mathematical, Physical and Engineering Sciences.
[37] Swinney,et al. Pattern formation in the presence of symmetries. , 1994, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.
[38] A. Thess,et al. Bénard–Marangoni convection at low Prandtl number , 1999, Journal of Fluid Mechanics.