Shock Waves and Reaction—Diffusion Equations pp 192-236 | Cite as
Systems of Reaction—Diffusion Equations
Chapter
Abstract
In recent years, systems of reaction-diffusion equations have received a great deal of attention, motivated by both their widespread occurrence in models of chemical and biological phenomena, and by the richness of the structure of their solution sets. In the simplest models, the equations take the form where u ∈ R n , D is an n x n matrix, and f(u) is a smooth function. The combination of diffusion terms together with the nonlinear interaction terms, produces mathematical features that are not predictable from the vantage point of either mechanism alone. Thus, the term DΔu acts in such a way as to “dampen” u, while the nonlinear function f(u) tends to produce large solutions, steep gradients, etc. This leads to the possibility of threshold phenomena, and indeed this is one of the interesting features of this class of equations.
$$ \frac{{\partial u}}{{\partial t}}{\mkern 1mu} = {\mkern 1mu} D\Delta u{\mkern 1mu} + {\mkern 1mu} f(u),\quad {\mkern 1mu} x \in {\mkern 1mu} \Omega {\mkern 1mu} \subset {\mkern 1mu} {R^k},{\mkern 1mu} t > {\mkern 1mu} 0, $$
(14.1)
Keywords
Vector Field Comparison Theorem Invariant Region General Boundary Condition Left Eigenvector
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.
Preview
Unable to display preview. Download preview PDF.
Copyright information
© Springer-Verlag New York Inc. 1983