Pattern formation in an N+Q component reaction-diffusion system.

A general N+Q component reaction-diffusion system is analyzed with regard to pattern forming instabilities (Turing bifurcations). The system consists of N mobile species and Q immobile species. The Q immobile species form in response to reactions between the N mobile species and an immobile substrate and allow the Turing instability to occur. These results are valid both for bifurcations from a spatially uniform state and for systems with an externally imposed gradient as in the experimental systems in which Turing patterns have been observed. It is shown that the critical wave number and the location of the instability in parameter space are independent of the substrate concentration. It is also found that the system necessarily undergoes a Hopf bifurcation as the total substrate concentration is decreased. Further, in the case that all the mobile species diffuse at identical rates we show that if the full system is at a point of Turing bifurcation then the N component mobile subsystem is at transition from an unstable focus to an unstable node, and the critical wave number is simply related to the degenerate positive eigenvalue of the mobile subsystem. A sequence of bifurcations that occur in the eigenspectra as the total substrate concentration is decreased to zero is also discussed.

[1]  Daniel R. Ripoll,et al.  Molecular model of the cooperative amylose-iodine-triiodide complex , 1986 .

[2]  I. Prigogine,et al.  On symmetry-breaking instabilities in dissipative systems , 1967 .

[3]  Linda E Reichl,et al.  Instabilities, Bifurcations, and Fluctuations in Chemical Systems , 1982 .

[4]  J. Murray How the Leopard Gets Its Spots. , 1988 .

[5]  J. Boissonade,et al.  Turing-type chemical patterns in the chlorite-iodide-malonic acid reaction , 1991 .

[6]  Zoltán Noszticzius,et al.  Effect of Turing pattern indicators on CIMA oscillators , 1992 .

[7]  A. Turing The chemical basis of morphogenesis , 1952, Philosophical Transactions of the Royal Society of London. Series B, Biological Sciences.

[8]  H. Swinney,et al.  Transition from a uniform state to hexagonal and striped Turing patterns , 1991, Nature.

[9]  I. Epstein,et al.  Modeling of Turing Structures in the Chlorite—Iodide—Malonic Acid—Starch Reaction System , 1991, Science.

[10]  Keiichi Tanaka,et al.  CO2 laser Stark spectroscopy of the ν4 band of SiHF3: The C0 rotational constant and vibrationally induced dipole moment , 1992 .

[11]  E. Sel'kov,et al.  Self-oscillations in glycolysis. 1. A simple kinetic model. , 1968, European journal of biochemistry.

[12]  Andrew Hodges,et al.  Alan Turing: The Enigma , 1983 .

[13]  Alan Garfinkel,et al.  Self-organizing systems : the emergence of order , 1987 .

[14]  Dulos,et al.  Experimental evidence of a sustained standing Turing-type nonequilibrium chemical pattern. , 1990, Physical review letters.

[15]  John E. Pearson,et al.  Pattern formation in a (2 + 1)-species activator-inhibitor-immobilizer system , 1992 .

[16]  Harry L. Swinney,et al.  Transition to chemical turbulence. , 1991, Chaos.

[17]  Axel Hunding,et al.  Size adaptation of turing prepatterns , 1988, Journal of mathematical biology.

[18]  J. Pearson,et al.  Turing instabilities with nearly equal diffusion coefficients , 1989 .

[19]  S A Kauffman,et al.  Control of sequential compartment formation in Drosophila. , 1978, Science.