A. Svirsky, T. Grafke, and A. Frishman
Abstract
Pipe flow is a canonical example of a subcritical flow, the
transition to turbulence requiring a finite perturbation. The
Reynolds number (Re) serves as the control parameter for this
transition, going from the ordered (laminar) to the chaotic
(turbulent) phase with increasing Re. Just above the critical Re,
where turbulence can be sustained indefinitely, turbulence spreads
via the self-replication of localized turbulent structures called
puffs. To reveal the workings behind this process, we consider
transitions between one and two-puff states, which dynamically are
transitions between two distinct chaotic saddles. We use direct
numerical simulations to explore the phase space boundary between
these saddles, adapting a bisection algorithm to identify an
attracting state on the boundary, termed an edge state. At Re=2200,
we also examine spontaneous transitions between the two saddles,
demonstrating the relevance of the found edge state to puff
self-replication. Our analysis reveals that the process of
self-replication follows a previously proposed splitting mechanism,
with the found edge state as its tipping point. Additionally, we
report results for lower values of Re, where the bisection algorithm
yields a different type of edge state. As we cannot directly observe
splits at this Re, the self-replication mechanism here remains an
open question. Our analysis suggests how this question could be
addressed in future studies, and paves the way to probing the
turbulence proliferation mechanism in other subcritical flows.
arXiv