Universal Dynamics of Damped-Driven Systems: The Logistic Map as a Normal Form for Energy Balance

TL;DR

This paper demonstrates that the universal instabilities in damped-driven systems can be modeled by a logistic map, providing a geometric framework that applies across diverse physical processes.

Contribution

It introduces a universal geometric description of energy balance in damped-driven systems, linking their dynamics to the logistic map and chaos theory.

Findings

Loss and gain curves intersect at energy-balanced solutions.

The system's dynamics are homeomorphic to the logistic map.

Universal period doubling and chaos emerge in these systems.

Abstract

Damped-driven systems are ubiquitous in engineering and science. Despite the diversity of physical processes observed in a broad range of applications, the underlying instabilities observed in practice have a universal characterization which is determined by the overall gain and loss curves of a given system. The universal behavior of damped-driven systems can be understood from a geometrical description of the energy balance with a minimal number of assumptions. The assumptions on the energy dynamics are as follows: the energy increases monotonically as a function of increasing gain, and the losses become increasingly larger with increasing energy, i.e. there are many routes for dissipation in the system for large input energy. The intersection of the gain and loss curves define an energy balanced solution. By constructing an iterative map between the loss and gain curves, the dynamics can be shown to be homeomorphic to the logistic map, which exhibits a period doubling cascade to chaos. Indeed, the loss and gain curves allow for a geometrical description of the dynamics through a simple Verhulst diagram (cobweb plot). Thus irrespective of the physics and its complexities, this simple geometrical description dictates the universal set of logistic map instabilities that arise in complex damped-driven systems. More broadly, damped-driven systems are a class of non-equilibrium pattern forming systems which have a canonical set of instabilities that are manifest in practice.