Suppression of chaos and other dynamical transitions induced by intercellular coupling in a model for cyclic AMP signaling in Dictyostelium cells.

The effect of intercellular coupling on the switching between periodic behavior and chaos is investigated in a model for cAMP oscillations in Dictyostelium cells. We first analyze the dynamic behavior of a homogeneous cell population which is governed by a three-variable differential system for which bifurcation diagrams are obtained as a function of two control parameters. We then consider the mixing of two populations behaving in a chaotic and periodic manner, respectively. Cells are coupled through the sharing of a common chemical intermediate, extracellular cAMP, which controls its production and release by the cells into the extracellular medium; the dynamics of the mixed suspension is governed by a five-variable differential system. When the two cell populations differ by the value of a single parameter which measures the activity of the enzyme that degrades extracellular cAMP, the bifurcation diagram established for the three-variable homogeneous population can be used to predict the dynamic behavior of the mixed suspension. The analysis shows that a small proportion of periodic cells can suppress chaos in the mixed suspension. Such a fragility of chaos originates from the relative smallness of the domain of aperiodic oscillations in parameter space. The bifurcation diagram is used to obtain the minimum fraction of periodic cells suppressing chaos. These results are related to the suppression of chaos by the small-amplitude periodic forcing of a strange attractor. Numerical simulations further show how the coupling of periodic cells with chaotic cells can produce chaos, bursting, simple periodic oscillations, or a stable steady state; the coupling between two populations at steady state can produce similar modes of dynamic behavior.

[1]  Reynolds,et al.  Streaming instability of aggregating slime mold amoebae. , 1991, Physical review letters.

[2]  A. Goldbeter,et al.  Origin of Bursting and Birhythmicity in a Model for Cyclic AMP Oscillations in Dictyostelium Cells , 1987 .

[3]  W. Loomis The Development of Dictyostelium Discoideum , 1982 .

[4]  G. Gerisch,et al.  Amplification of cyclic‐AMP signals in aggregating cells of Dictyostelium discoideum , 1975, FEBS letters.

[5]  A Goldbeter,et al.  Birhythmicity, chaos, and other patterns of temporal self-organization in a multiply regulated biochemical system. , 1982, Proceedings of the National Academy of Sciences of the United States of America.

[6]  G. Ermentrout Oscillator death in populations of “all to all” coupled nonlinear oscillators , 1990 .

[7]  G. Ermentrout,et al.  Oscillator death in systems of coupled neural oscillators , 1990 .

[8]  G. Gerisch Cyclic AMP and other signals controlling cell development and differentiation in Dictyostelium. , 1987, Annual review of biochemistry.

[9]  G. Gerisch,et al.  Intracellular oscillations and release of cyclic AMP from Dictyostelium cells. , 1975, Biochemical and biophysical research communications.

[10]  E. Lorenz Dimension of weather and climate attractors , 1991, Nature.

[11]  Frank H. Eeckman,et al.  Analysis and Modeling of Neural Systems , 1992, Springer US.

[12]  S. Strogatz,et al.  Amplitude death in an array of limit-cycle oscillators , 1990 .

[13]  Arkady Pikovsky,et al.  On the interaction of strange attractors , 1984 .

[14]  A. Durston Pacemaker mutants of Dictyostelium discoideum. , 1974, Developmental biology.

[15]  A. Arneodo,et al.  Oscillatory instability induced by mass interchange between two coupled steady-state reactors , 1987 .

[16]  P. Devreotes,et al.  Adenosine 3',5'-monophosphate waves in Dictyostelium discoideum: a demonstration by isotope dilution--fluorography. , 1981, Science.

[17]  A. Goldbeter,et al.  Birhythmicity in a model for the cyclic AMP signalling system of the slime mold Dictyostelium discoideum , 1985 .

[18]  K. Bar-Eli,et al.  Coupling of chemical oscillators , 1984 .

[19]  M. B. Coukell,et al.  The precocious appearance and activation of an adenylate cyclase in a rapid developing mutant of Dictyostelium discoideum , 1980, FEBS letters.

[20]  L. Olsen,et al.  Chaos in biological systems. , 1985 .

[21]  Michael F. Crowley,et al.  Experimental and theoretical studies of a coupled chemical oscillator: phase death, multistability, and in-phase and out-of-phase entrainment , 1989 .

[22]  A. Goldbeter,et al.  Autonomous chaotic behaviour of the slime mould Dictyostelium discoideum predicted by a model for cyclic AMP signalling , 1985, Nature.

[23]  Hans G. Othmer,et al.  An analytical and numerical study of the bifurcations in a system of linearly-coupled oscillators , 1987 .

[24]  John J. Tyson,et al.  Spiral waves of cyclic amp in a model of slime mold aggregation , 1989 .

[25]  L. Glass,et al.  From Clocks to Chaos: The Rhythms of Life , 1988 .

[26]  Agnessa Babloyantz,et al.  Pacemaker-Induced Coherence in Cortical Networks , 1991, Neural Computation.

[27]  C. Weijer,et al.  In situ measurements of external pH and optical density oscillations in Dictyostelium discoideum aggregates , 1986, The Journal of cell biology.

[28]  A Goldbeter,et al.  A Model Based on Receptor Desensitization for Cyclic AMP Signaling in Dictyostelium Cells. , 1987, Biophysical journal.

[29]  I. Epstein,et al.  Systematic design of chemical oscillators. Part 19. Experimental study of complex dynamical behavior in coupled chemical oscillators , 1984 .

[30]  Goldhirsch,et al.  Taming chaotic dynamics with weak periodic perturbations. , 1991, Physical review letters.

[31]  F. Alcântara,et al.  Signal propagation during aggregation in the slime mould Dictyostelium discoideum. , 1974, Journal of general microbiology.