paper

Time Dependent Saddle Node Bifurcation: Breaking Time and the Point of No Return in a Non-Autonomous Model of Critical Transitions

arXiv:1611.09542 · doi:10.1016/j.physd.2019.02.005

Abstract

There is a growing awareness that catastrophic phenomena in biology and medicine can be mathematically represented in terms of saddle-node bifurcations. In particular, the term `tipping', or critical transition has in recent years entered the discourse of the general public in relation to ecology, medicine, and public health. The saddle-node bifurcation and its associated theory of catastrophe as put forth by Thom and Zeeman has seen applications in a wide range of fields including molecular biophysics, mesoscopic physics, and climate science. In this paper, we investigate a simple model of a non-autonomous system with a time-dependent parameter and its corresponding `dynamic' (time-dependent) saddle-node bifurcation by the modern theory of non-autonomous dynamical systems. We show that the actual point of no return for a system undergoing tipping can be significantly delayed in comparison to the {\em breaking time} at which the corresponding autonomous system with a time-independent parameter undergoes a bifurcation. A dimensionless parameter is introduced, in which is the curvature of the autonomous saddle-node bifurcation according to parameter , which has an initial value of and a constant rate of change . We find that the breaking time is always less than the actual point of no return after which the critical transition is irreversible; specifically, the relation is analytically obtained. For a system with a small , there exists a significant window of opportunity during which rapid reversal of the environment can save the system from catastrophe.

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