SearcharxivSearch

arXiv · 1605.08258

Pattern formation in a pseudo-parabolic equation

Abstract

We address the propagation into an unstable state of a localised disturbance in a forward-backward diffusion pseudo-parabolic equation. Three asymptotic regimes are distinguished as t tends to infinity, the first being a regime ahead of the propagating disturbance that is dominated by the linearised equation. The analysis of this leads to the determination of the speed of the leading edge of the propagating disturbance and implies that in the second, transition, regime the solution takes the form of a modulated travelling wave. In a third regime the solution approaches a nearly periodic steady state, where the period is obtained on matching with the modulated travelling wave. Detailed analysis of this pattern is also presented. The analysis is completed by contrasting the formal asymptotic description of the solution with numerical computations. It is assumed for the above analysis that the initial disturbance decays faster than an exponential rate; in this case a critical exponential decay rate at the leading edge of the front and propagation speed are found. We investigate the wave speed selection mechanism for exponentially decaying initial conditions. It is found that whenever the initial data behave as a real exponential (no matter how slow the rate of the decay) the speed selected is that selected by fast decaying initial conditions. However, for initial conditions with a complex exponential we find regimes of the decay rate and the wavelength for which the front propagates at a faster wave speed. This is investigated numerically and is worth emphasising since it gives a different scenario for wave speed behaviour than that exhibited by well-studied semilinear reaction-diffusion equations: there are initial conditions with exponential decay faster than the critical one for which the front propagates with a speed faster than the critical one.

Explore related subjects

Keep this discovery

BibTeXRIS

C. M. Cuesta, J. R. King. 2016-05-26. Pattern formation in a pseudo-parabolic equation. https://arxiv.org/abs/1605.08258

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Well-posedness of the two-dimensional unsteady Prandtl system in Sobolev space with degenerate critical points

This paper is devoted to the well-posedness of classical Prandtl equations in a finite order Sobolev space. For a initial data with degenerate critical points and general outflow, we obtain the local-in-time existence and uniqueness of the solution to the Prandtl equations in a Sobolev space, by introducing a new iteration scheme and linear cancelation. This result shows that Oleinik's monotonicity condition is not a necessary condition for the Prandtl equations to be well-posed in Sobolev spaces and provides evidence to demonstrate that zero shear stress does not necessarily lead to boundary layer separation in two-dimensional unsteady boundary layers.

math.AP

Global existence and time decay for a bipolar Euler-Poisson system with one pressureless and undamped fluid

We study the Cauchy problem for a three-dimensional bipolar Euler--Poisson system in which one fluid is pressureless and undamped, while the other is subject to momentum relaxation. For sufficiently small smooth perturbations of a constant equilibrium, we prove the global existence and uniqueness of smooth solutions under an irrotationality assumption on the initial velocity of the pressureless fluid, together with algebraic time-decay estimates. The main difficulty is that the velocity of the pressureless fluid is dissipated only indirectly through the Poisson coupling, and this mechanism degenerates strongly at high frequencies, leading to a regularity-loss structure. We overcome this difficulty by combining refined Green-function estimates, a low--middle--high frequency decomposition, and high-order nonlinear energy estimates adapted to the asymmetric regularity hierarchy. The result establishes a global small-data theory for this asymmetric regime, in which pressure and damping are simultaneously absent from the same fluid.

math.AP

Boundary layer of 2D Chemotaxis Navier-Stokes equations with logarithmic Sensitivity. II. viscous vanishing limit

This is the second part of a two-part work concerning boundary layer solutions to the coupled Chemotaxis-Navier-Stokes system in the two-dimensional half-space. In the present work, we address the convergence of boundary layer solutions to singular chemotaxis-fluid equations under slip boundary conditions with respect to the chemical diffusion-viscosity parameter $\varepsilon$ in the two-dimensional half-plane. More precisely, we show that the boundary layer for $\varepsilon>0$ (viscous convection coefficient) converges to the superposition of the outer layer (solution with $\varepsilon=0$) and the inner layer as $\varepsilon\rightarrow0$. The outer and inner profiles are explicitly derived as in the first part\cite{WWZ}. Furthermore, the well-posedness results of the coupled Chemotaxis-Navier-Stokes system in conormal Sobolev spaces will be presented in Appendix. They answer the question mentioned in the first part of the two-part work. This study could help the understanding of the chemotactic movement of aerobic bacteria to the water-air surface observed experimentally in fluids, and enrich the theoretical results of boundary layer in chemotactic fluid models.

math.AP