On long-time dynamics for competition-diffusion systems with inhomogeneous Dirichlet boundary conditions (original) (raw)

Singular limit of a competition–diffusion system with large interspecific interaction

Journal of Mathematical Analysis and Applications, 2012

We consider a competition-diffusion system for two competing species; the density of the first species satisfies a parabolic equation together with a inhomogeneous Dirichlet boundary condition whereas the second one either satisfies a parabolic equation with a homogeneous Neumann boundary condition, or an ordinary differential equation. Under the situation where the two species spatially segregate as the interspecific competition rate becomes large, we show that the resulting limit problem turns out to be a free boundary problem. We focus on the singular limit of the interspecific reaction term, which involves a measure located on the free boundary.

Instability of non-constant equilibrium solutions of a system of competition-diffusion equations

Journal of Mathematical Biology, 1981

The system of interaction-diffusion equations describing competition between two species is investigated. By using a version of the Perron-Frobenius theorem of positive matrices generalized to function spaces, it is proved that any non-constant equilibrium solution of the system is unstable both under Neumann boundary conditions (for the rectangular parallelepiped domain) and under periodic conditions. It is conjectured that this result extends to convex domains, and that the simple interaction-diffusion model cannot explain spatially segregated distributions of two competing species in such domains.

On stable space dependent stationary solutions of a competition system with diffusion

Zeitschrift für Analysis und ihre Anwendungen, 1983

Zeithchrift fUr,Anaiysis und ihre Anwendungen Bd.2 (3) 1983, S. 193-206 'i.neu it nocTaB.neiio icpaeoe yeioBue J.IipBxe. 14ccJ1e1y1oTcH 6. 11(flypKatum nO.nO?IuITcJIbHIJx cT611lIoHuI)HbIX peiueiiii xapaep ttx ac1lM[1TOTi 11ecHofl VCTOfI'I1IBOCTII it lix 3anuduMocm OT lipocTpaEicTBeHHou nepelielluoll. A quasilinear parabolic system of two equations is considered, only one of which includes the diffusionrni. The bifurcation of nonnegative stationary solutions is studied together with their stability character and their dependence on the "space" variables.

A reaction-diffusion-advection competition model with a free boundary

In this paper, we study a competitive diffusion quasilinear system with a free boundary. First, we investigate the mathematical questions of the problem. A priori estimates of Schauder type are established, which are necessary for the solvability of the problem. One of two competing species is an invader, which initially exists on a certain sub-interval. The other is initially distributed throughout the area under consideration. Examining the influence of baseline data on the success or failure of the first invasion. We conclude that there is a dichotomy of spread and extinction and give precise criteria for spread and extinction in this model.

Spatial segregation limit of a competition–diffusion system

European Journal of Applied Mathematics, 1999

We consider a competition–diffusion system and study its singular limit as the interspecific competition rate tend to infinity. We prove the convergence to a Stefan problem with zero latent heat.

Singular Limit of a Spatially Inhomogeneous Lotka–Volterra Competition–Diffusion System

Communications in Partial Differential Equations, 2007

We discuss the generation and the motion of internal layers for a Lotka-Volterra competition-diffusion system with spatially inhomogeneous coefficients. We assume that the corresponding ODE system has two stable equilibria ū 0 and 0 v with equal strength of attraction in the sense to be specified later. The equation involves a small parameter , which reflects the fact that the diffusion is very small compared with the reaction terms. When the parameter is very small, the solution develops a clear transition layer between the region where the u species is dominant and the one where the v species is dominant. As tends to zero, the transition layer becomes a sharp interface, whose motion is subject to a certain law of motion, which is called the "interface equation". A formal asymptotic analysis suggests that the interface equation is the motion by mean curvature coupled with a drift term.

On nonlinear coupled diffusions in competition systems

Nonlinear Analysis-real World Applications, 2012

A class of reaction-diffusion systems modeling plant growth with spatial competition in saturated media is presented. We show, in this context, that standard diffusion can not lead to pattern formation (Diffusion Driven Instability of Turing). Degenerated nonlinear coupled diffusions inducing free boundaries and exclusive spatial diffusions are proposed. Local and global existence results are proved for smooth approximations of the degenerated nonlinear diffusions systems which give rise to long-time pattern formations. Numerical simulations of a competition model with degenerate/non degenerate nonlinear coupled diffusions are performed and we carry out the effect of the these diffusions on pattern formation and on the change of basins of attraction.

Long-term coexistence for a competitive system of spatially varying gradient reaction–diffusion equations

Nonlinear Analysis: Real World Applications, 2009

Spatial distribution of interacting chemical or biological species is usually described by a system of reaction-diffusion equations. In this work we consider a system of two reactiondiffusion equations with spatially varying diffusion coefficients which are different for different species and with forcing terms which are the gradient of a spatially varying potential. Such a system describes two competing biological species. We are interested in the possibility of long-term coexistence of the species in a bounded domain. Such long-term coexistence may be associated either with a periodic in time solution (usually associated with a Hopf bifurcation), or with time-independent solutions. We prove that no periodic solution exists for the system. We also consider some steady-states (the time-independent solutions) and examine their stability and bifurcations.