Pattern formation with a conservation law

Pattern formation in systems with a conserved quantity is considered by studying the appropriate amplitude equations. The conservation law leads to a large-scale neutral mode that must be included in the asymptotic analysis for pattern formation near onset. Near a stationary bifurcation, the usual Ginzburg--Landau equation for the amplitude of the pattern is then coupled to an equation for the large-scale mode. These amplitude equations show that for certain parameters all roll-type solutions are unstable. This new instability differs from the Eckhaus instability in that it is amplitude-driven and is supercritical. Beyond the stability boundary, there exist stable stationary solutions in the form of strongly modulated patterns. The envelope of these modulations is calculated in terms of Jacobi elliptic functions and, away from the onset of modulation, is closely approximated by a sech profile. Numerical simulations indicate that as the modulation becomes more pronounced, the envelope broadens. A number of applications are considered, including convection with fixed-flux boundaries and convection in a magnetic field, resulting in new instabilities for these systems.

[1]  Riecke Self-trapping of traveling-wave pulses in binary mixture convection. , 1992, Physical review letters.

[2]  H. Sakaguchi Phase Dynamics and Localized Solutions to the Ginzburg-Landau Type Amplitude Equations , 1993 .

[3]  P. Matthews Asymptotic solutions for nonlinear magnetoconvection , 1999, Journal of Fluid Mechanics.

[4]  Matthews,et al.  One-dimensional pattern formation with galilean invariance near a stationary bifurcation , 2000, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[5]  Stephen M. Cox,et al.  Instability of rotating convection , 2000, Journal of Fluid Mechanics.

[6]  Coullet,et al.  Instabilities of one-dimensional cellular patterns. , 1990, Physical review letters.

[7]  Soft-mode turbulence in electrohydrodynamic convection of a homeotropically aligned nematic layer , 1997 .

[8]  Edmund Taylor Whittaker,et al.  A Course of Modern Analysis , 2021 .

[9]  C. J. Chapman,et al.  Nonlinear Rayleigh–Bénard convection between poorly conducting boundaries , 1980, Journal of Fluid Mechanics.

[10]  Coullet,et al.  Propagative phase dynamics for systems with Galilean invariance. , 1985, Physical review letters.

[11]  H. Sakaguchi,et al.  Stable localized solutions of arbitrary length for the quintic Swift-Hohenberg equation , 1996 .

[12]  Stephen M. Cox,et al.  Long-Wavelength Rotating Convection Between Poorly Conducting Boundaries , 1998, SIAM J. Appl. Math..

[13]  Hermann Riecke,et al.  Localization of waves without bistability: Worms in nematic electroconvection , 1998 .

[14]  S. Chandrasekhar Hydrodynamic and Hydromagnetic Stability , 1961 .

[15]  L. Tuckerman,et al.  Bifurcation analysis of the Eckhaus instability , 1990 .

[16]  I. Melbourne Steady-state bifurcation with Euclidean symmetry , 1999 .

[17]  F. Charru,et al.  Benjamin-feir and eckhaus instabilities with galilean invariance: the case of interfacial waves in viscous shear flows , 1998 .

[18]  Hermann Riecke Ginzburg-Landau equation coupled to a concentration field in binary-mixture convection , 1992 .

[19]  M. Cross,et al.  Pattern formation outside of equilibrium , 1993 .

[21]  Michael F. Schatz,et al.  Long-wavelength surface-tension-driven Bénard convection: experiment and theory , 1997, Journal of Fluid Mechanics.

[22]  F. Charru,et al.  Secondary instabilities of interfacial waves due to coupling with a long wave mode in a two-layer Couette flow , 1999 .

[23]  Schatz,et al.  Long-wavelength instability in surface-tension-driven Bénard convection. , 1995, Physical review letters.

[24]  P. Matthews Hexagonal patterns in finite domains , 1997, patt-sol/9703002.

[25]  Tsuboi,et al.  New scenario for transition to turbulence? , 1996, Physical review letters.

[26]  W. Eckhaus Studies in Non-Linear Stability Theory , 1965 .

[27]  Hermann Riecke Solitary waves under the influence of a long-wave mode , 1996 .

[28]  Velarde,et al.  Short-wavelength instability in systems with slow long-wavelength dynamics. , 1996, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[29]  J. Swift,et al.  Hydrodynamic fluctuations at the convective instability , 1977 .

[30]  Anthony J. Roberts,et al.  An analysis of near-marginal, mildly penetrative convection with heat flux prescribed on the boundaries , 1985, Journal of Fluid Mechanics.

[31]  L. Pismen,et al.  Interaction between short‐scale Marangoni convection and long‐scale deformational instability , 1994 .

[32]  P. Matthews A model for the onset of penetrative convection , 1988, Journal of Fluid Mechanics.