Wavy film flows down an inclined plane. Part I: Perturbation theory and general evolution equation for the film thicknessWavy film flow of incompressible Newtonian fluid down an inclined plane is considered. The question is posed as to the parametric conditions under which the description of evolution can be…Alexander L. Frenkel, Keshavamurthy Indireshkumar·Dec 15, 1997SaveLearn
The dynamics of vortex lines in the three-dimensional complex Ginzburg-Landau equation: instability, stretching, entanglement, and helicesThe dynamics of curved vortex filaments is studied analytically and numerically in the framework of a three-dimensional complex Ginzburg-Landau equation (CGLE). It is shown that a straight vortex…I. S. Aranson, A. R. Bishop, L. Kramer·Dec 9, 1997SaveLearn
Amplitude equations and pattern selection in Faraday wavesA nonlinear theory of pattern selection in parametric surface waves (Faraday waves) is presented that is not restricted to small viscous dissipation. By using a multiple scale asymptotic expansion…Peilong Chen, Jorge Vinals·Dec 8, 1997SaveLearn
Phase chaos in the anisotropic complex Ginzburg-Landau EquationOf the various interesting solutions found in the two-dimensional complex Ginzburg-Landau equation for anisotropic systems, the phase-chaotic states show particularly novel features. They exist in a…R. Faller, L. Kramer·Dec 4, 1997SaveLearn
Adiabatic reduction near a bifurcation in stochastically modulated systemsWe re-examine the procedure of adiabatic elimination of fast relaxing variables near a bifurcation point when some of the parameters of the system are stochastically modulated. Approximate stationary…Francois Drolet, Jorge Vinals·Dec 3, 1997SaveLearn
Propagation failure of traveling waves in a discrete bistable mediumPropagation failure (pinning) of traveling waves is studied in a discrete scalar reaction-diffusion equation with a piecewise linear, bistable reaction function. The critical points of the pinning…Gabor Fath·Nov 20, 1997SaveLearn
Introduction to Extended ElectrodynamicsThis paper summarizes the motivations and results obtained so far in the frame of a particular non-linearization of Classical Electrodynamics, which was called Extended Electrodynamics. The main…Stoil Donev·Nov 14, 1997SaveLearn
Mutator Dynamics on a Smooth Evolutionary LandscapeWe investigate a model of evolutionary dynamics on a smooth landscape which features a ``mutator'' allele whose effect is to increase the mutation rate. We show that the expected proportion…David A. Kessler, Herbert Levine·Nov 2, 1997SaveLearn
Annular electroconvection with shearWe report experiments on convection driven by a radial electrical force in suspended annular smectic A liquid crystal films. In the absence of an externally imposed azimuthal shear, a stationary…Zahir A. Daya, V. B. Deyirmenjian, Stephen W. Morris et al.·Oct 9, 1997SaveLearn
Nonlinear Competition Between Small and Large Hexagonal PatternsRecent experiments by Kudrolli, Pier and Gollub on surface waves, parametrically excited by two-frequency forcing, show a transition from a small hexagonal standing wave pattern to a triangular…Mary Silber, Michael R. E. Proctor·Oct 8, 1997SaveLearn
Extended Electrodynamics: III. Free Photons and (3+1)-Soliton- like Vacuum SolutionsThis paper aims to give explicitly all non-linear vacuum solutions to our non-linear field equations, and to define in a coordinate free manner the important subclass of non-linear solutions, which…S. Donev, M. Tashkova·Oct 6, 1997SaveLearn
Propagation Failure in Excitable MediaWe study a mechanism of pulse propagation failure in excitable media where stable traveling pulse solutions appear via a subcritical pitchfork bifurcation. The bifurcation plays a key role in that…Aric Hagberg, Ehud Meron·Oct 3, 1997SaveLearn
Extended Electrodynamics: II. Properties and invariant characteristics of the non-linear vacuum solutionsThis paper aims to consider the general properties of the non-linear solutions to the vacuum equations of Extended Electrodynamics. The *-invariance and the conformal invariance of the equations are…S. Donev, M. Tashkova·Oct 3, 1997SaveLearn
Extended Electrodynamics I. Basic Notions, Principles and EquationsThis paper aims to present an elaborate view on the motivation and realization of the idea to extend Maxwell's electrodynamics to Extended Electrodynamics in a reasonable and appropriate way in…S. Donev, M. Tashkova·Oct 2, 1997SaveLearn
Spiral Motion in a Noisy Complex Ginzburg-Landau EquationThe response of spiral waves to external perturbations in a stable regime of the two-dimensional complex Ginzburg-Landau equation (CGLE) is investigated. It is shown that the spiral core has a finite…Igor Aranson, Hugues Chate, Lei Han Tang·Sep 25, 1997SaveLearn
Kinematic Equations for Front Motion and Spiral-Wave NucleationWe present a new set of kinematic equations for front motion in bistable media. The equations extend earlier kinematic approaches by coupling the front curvature with the order parameter associated…Aric Hagberg, Ehud Meron·Sep 23, 1997SaveLearn
Uses of Envelopes for Global and Asymptotic Analysis; geometrical meaning of renormalization group equationWe give a comprehensive review of the renormalization group method for global and asymptotic analysis, putting an emphasis on the relevance to the classical theory of envelopes and the existence of…Teiji Kunihiro·Sep 20, 1997SaveLearn
Localized moving breathers in a 2-D hexagonal latticeWe show for the first time that highly localized in-plane breathers can propagate in specific directions with minimal lateral spreading in a model 2-D hexagonal non-linear lattice. The lattice is…J. L. Marín, J. C. Eilbeck, F. M. Russell·Sep 17, 1997SaveLearn
Complexation of Wavenumbers in SolitonsIt is shown that, by letting wavenumbers and frequencies complex in Hirota's bilinear method, new classes of exact solutions of soliton equations can be obtained systematically. They include not…M. Umeki·Sep 3, 1997SaveLearn
Amplitude equations for coupled electrostatic waves in the limit of weak instabilityWe consider the simplest instabilities involving multiple unstable electrostatic plasma waves corresponding to four-dimensional systems of mode amplitude equations. In each case the coupled amplitude…John David Crawford, Edgar Knobloch·Aug 21, 1997SaveLearn
Spatio-temporal dynamics of coupled array of Murali-Lakshmanan-Chua circuitsThe circuit recently proposed by Murali, Lakshmanan and Chua (MLC) is one of the simplest non-autonomous nonlinear electronic circuits which shows a variety of dynamical phenomena including various…P. Muruganandam, K. Murali, M. Lakshmanan·Aug 20, 1997SaveLearn
Nature of Roll to Spiral-Defect-Chaos TransitionWe investigate the nature of the parallel-roll to spiral-defect-chaos (SDC) transition in Rayleigh-Benard convection, based on the generalized Swift-Hohenberg model. We carry out extensive,…Xiao-jun Li, Hao-wen Xi, J. D. Gunton·Aug 12, 1997SaveLearn
Noise sustained pattern growth: Bulk versus boundary effectsThe effect of thermally generated bulk stochastic forces on the statistical growth dynamics of forwards bifurcating propagating macroscopic patterns is compared with the influence of fluctuations at…M. Luecke, A. Szprynger·Aug 6, 1997SaveLearn
Order Parameter Equations for Front Transitions: Nonuniformly Curved FrontsKinematic equations for the motion of slowly propagating, weakly curved fronts in bistable media are derived. The equations generalize earlier derivations where algebraic relations between the normal…Aric Hagberg, Ehud Meron·Jul 29, 1997SaveLearn
Strongly nonlinear convection in binary fluids: Minimal model for extended states using symmetry decomposed modesSpatially extended stationary and traveling states in the strongly nonlinear regime of convection in layers of binary fluid mixtures heated from below are described by a few-mode-model. It is derived…St. Hollinger, M. Luecke·Jul 29, 1997SaveLearn