Abstract

Dissipative dynamical systems characterised by two basins of attraction are found in many physical systems, notably in hydrodynamics where laminar and turbulent regimes can coexist. The state space of such systems is structured around a dividing manifold called the edge, which separates trajectories attracted by the laminar state from those reaching the turbulent state. We apply here concepts and tools from Lagrangian data analysis to investigate this edge manifold. This approach is carried out in the state space of automous arbitrarily high-dimensional dissipative systems, in which the edge manifold is re-interpreted as a Lagrangian Coherent Structure (LCS). Two different diagnostics, finite-time Lyapunov exponents and Lagrangian Descriptors, are used and compared with respect to their ability to identify the edge and to their scalability. Their properties are illustrated on several low-order models of subcritical transition of increasing dimension and complexity, as well on well-resolved simulations of the Navier-Stokes equations in the case of plane Couette flow. They allow for a mapping of the global structure of both the state space and the edge manifold based on quantitative information. Both diagnostics can also be used to generate efficient bisection algorithms to approach asymptotic edge states, which outperform classical edge tracking.

Highlights

  • Many deterministic physical systems can operate in two different regimes depending on initial conditions

  • Reference [45] provides rigorous theorems that establish a precise connection between hyperbolic Lagrangian coherent structure (LCS) and finite-time Lyapunov exponents (FTLEs) ridges when further conditions on the rate-of-strain tensor are satisfied along the ridges

  • These results show that the edge manifold is again highlighted as a repelling LCS in a nonchaotic case when neither the edge state nor the turbulent attractor are fixed points

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Summary

INTRODUCTION

Many deterministic physical systems can operate in two different regimes depending on initial conditions. In the Eulerian point of view relevant to the transition problem, both spaces differ radically in their dimension It is in line with the point of view used first by Ref. We suggest and test the use of these diagnostics to improve edge tracking algorithms

DEFINITIONS AND LCS DIAGNOSTICS
Finite-time Lyapunov exponents
Lagrangian descriptors
LCS IDENTIFICATION OF THE EDGE
Hierarchy of low-order shear flow models
Navier-Stokes equations
EDGE TRACKING REVISITED
Global versus local methods
Comparison of different methods for edge tracking
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