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Modeling the collapse of the edge when two transition routes compete
KTH, School of Engineering Sciences (SCI), Centres, Linné Flow Center, FLOW. KTH, School of Engineering Sciences (SCI), Engineering Mechanics, Vehicle Engineering and Solid Mechanics, Stability, Transition and Control. KTH, Centres, SeRC - Swedish e-Science Research Centre.ORCID iD: 0000-0002-4045-7262
LIMSI-CNRS, Université Paris-Saclay, P91405 Orsay, France.ORCID iD: 0000-0001-6258-0475
KTH, School of Engineering Sciences (SCI), Centres, Linné Flow Center, FLOW. KTH, School of Engineering Sciences (SCI), Engineering Mechanics, Vehicle Engineering and Solid Mechanics, Stability, Transition and Control. KTH, Centres, SeRC - Swedish e-Science Research Centre.ORCID iD: 0000-0001-7864-3071
2020 (English)In: Physical review. E, ISSN 2470-0045, E-ISSN 2470-0053, Vol. 102, no 5, article id 053108Article in journal (Refereed) Published
Abstract [en]

The transition to turbulence in many shear flows proceeds along two competing routes, one linked with finite-amplitude disturbances and the other one originating from a linear instability, as in, e.g., boundary layer flows. The dynamical systems concept of an edge manifold has been suggested in the subcritical case to explain the partition of the state space of the system. This investigation is devoted to the evolution of the edge manifold when linear stability is added in such subcritical systems, a situation poorly studied despite its prevalence in realistic fluid flows. In particular, the fate of the edge state as a mediator of transition is unclear. A deterministic three-dimensional model is suggested, parametrized by the linear instability growth rate. The edge manifold evolves topologically, via a global saddle-loop bifurcation of the underlying invariant sets, from the separatrix between two attraction basins to the mediator between two transition routes. For larger instability rates, the stable manifold of the saddle point increases in codimension from 1 to 2 after an additional local pitchfork node bifurcation, causing the collapse of the edge manifold. As the growth rate is increased, three different regimes of this model are identified, each one associated with a flow case from the recent hydrodynamic literature. A simple nonautonomous generalization of the model is also suggested in order to capture the complexity of spatially developing flows.

Place, publisher, year, edition, pages
American Physical Society (APS) , 2020. Vol. 102, no 5, article id 053108
National Category
Fluid Mechanics and Acoustics
Identifiers
URN: urn:nbn:se:kth:diva-287788DOI: 10.1103/PhysRevE.102.053108ISI: 000594838300018PubMedID: 33327071Scopus ID: 2-s2.0-85097580880OAI: oai:DiVA.org:kth-287788DiVA, id: diva2:1522701
Note

QC 20210126

Available from: 2021-01-26 Created: 2021-01-26 Last updated: 2022-06-25Bibliographically approved
In thesis
1. Nonlinear dynamics in transitional wall-bounded flows
Open this publication in new window or tab >>Nonlinear dynamics in transitional wall-bounded flows
2021 (English)Doctoral thesis, comprehensive summary (Other academic)
Alternative title[sv]
Icke-linjär dynamik i vägg-bunden strömning
Abstract [en]

This thesis focuses on numerical studies of subcritical transition to turbulence in shear flows. The thesis employs a framework based on nonlinear dynamics in the subsequent studies. The geometrical approach to subcritical transition pivots the concepts of edge manifold and edge state. Such concepts are explored in detail in the Blasius boundary layer. The identified edge trajectory is chaotic and presents a couple of high- and low-speed streaks akin to those identified in other shear flows. For long enough times the linear instability of the Blasiusboundary layer coexists with the bypass transition scenario. The edge is thus reinterpreted as a manifold separating both routes. On the edge manifold of the Blasius boundary layer, the fully localised minimal seed is identified. The minimal seed experiences a sequence of linear mechanisms: the Orr mechanism followed by the lift-up. The resulting perturbation approaches the same region in state space as identified from arbitrary perturbations.These insights from the edge trajectory identified in the Blasius boundary layer inspired a low-dimensional model. The model illustrates the e↵ect of the laminar attractor becoming linearly unstable and it agrees qualitatively withother recent studies in the literature.The edge has been identified as a hyperbolic Lagrangian coherent structure of infinite dimension. We show how two Lagrangian diagnostics can be used to locate the edge directly in state space. This allows us to revisit edge tracking as a method optimising a Lagrangian diagnostic instead of a binary algorithm.The two last studies of the thesis focus on the optimally time-dependent(OTD) modes as a basis for the linearised dynamics about a base flow with arbitrary time-dependence. The OTD modes are explored for a periodic flow in pulsating plane Poiseuille flow. The resulting OTD modes can be linked to thespectrum of the Orr-Sommerfeld operator. The results revealed perturbations which span more than one period of the base flow. Finally, the OTD frameworkis used on the edge trajectory starting from the minimal seed in the Blasiusboundary layer.

Place, publisher, year, edition, pages
Stockholm: KTH Royal Institute of Technology, 2021. p. 69
Series
TRITA-SCI-FOU ; 2021:017
National Category
Fluid Mechanics and Acoustics
Research subject
Engineering Mechanics
Identifiers
urn:nbn:se:kth:diva-294298 (URN)978-91-7873-899-1 (ISBN)
Public defence
2021-06-04, Live-streamiing via Zoom: https://kth-se.zoom.us/j/62902876216, Stockholm, 10:00 (English)
Opponent
Supervisors
Funder
Swedish Research Council, 2016-03541
Available from: 2021-05-17 Created: 2021-05-14 Last updated: 2022-06-25Bibliographically approved

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Beneitez Galan, MiguelHenningson, Dan S.

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