Unstable manifolds computation for the two-dimensional plane Poiseuille flow

In this work we study some aspects of the dynamics of the plane Poiseuille problem in dimension 2, in what refers to the connection among different configurations of the flow. The fluid is confined in a channel of plane parallel walls. The problem is modeled by the incompressible Navier-Stokes equat...

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Detalles Bibliográficos
Autores: Sánchez Casas, José Pablo, Jorba, Angel
Tipo de recurso: artículo
Fecha de publicación:2003
País:España
Institución:Universitat Politècnica de Catalunya (UPC)
Repositorio:UPCommons. Portal del coneixement obert de la UPC
Idioma:inglés
OAI Identifier:oai:upcommons.upc.edu:2117/899
Acceso en línea:https://hdl.handle.net/2117/899
Access Level:acceso abierto
Palabra clave:Differentiable dynamical systems
Fluid mechanics
Poiseuille flow
Unstable manifolds computation
Sistemes dinàmics diferenciables
Teoria ergòdica
Fluids
Vorticitat -- Teoria
Classificació AMS::76 Fluid mechanics::76D Incompressible viscous fluids
Classificació AMS::37 Dynamical systems and ergodic theory::37N Applications
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spelling Unstable manifolds computation for the two-dimensional plane Poiseuille flowSánchez Casas, José PabloJorba, AngelDifferentiable dynamical systemsFluid mechanicsPoiseuille flowUnstable manifolds computationSistemes dinàmics diferenciablesTeoria ergòdicaFluidsVorticitat -- TeoriaClassificació AMS::76 Fluid mechanics::76D Incompressible viscous fluidsClassificació AMS::37 Dynamical systems and ergodic theory::37N ApplicationsIn this work we study some aspects of the dynamics of the plane Poiseuille problem in dimension 2, in what refers to the connection among different configurations of the flow. The fluid is confined in a channel of plane parallel walls. The problem is modeled by the incompressible Navier-Stokes equations ∂u ∂t + (u · ∇)u = −∇p + 1 Re ∆u, ∇ · u = 0, (1) being Re the Reynolds number, together with no-slip on the channel walls and L-periodic boundary conditions (L = 2π/α, being α the parameter wave number). We have considered two different formulations to drive the fluid through the channel: holding constant the total flux or the mean pressure gradient. For each of them we obtain a different definition of Re = hUc/ν, where h represents half of the channel length, Uc the velocity of the laminar flow in the centre of the channel, and ν the kinematic viscosity. To be precise ReQ = 3Q/ν, Rep = Gh3ρ/2µ2, corresponds to the Reynolds numbers when we keep Q as a constant flux or G as a constant mean pressure gradient respectively. The fluid is supposed of constant density ρ and viscosity µ. The numerical approximation is detailed in [1]. Roughly, it employs Fourier and Chebyshev spectral discretizations of velocities and pressure in the periodic and transversal directions respectively. The temporal variable is approximated by means of finite differences. In figure 1 we represent bifurcating curves of periodic and quasi-periodic flows obtained numerically in [1] using N = 8 and M = 70 spectral modes in the x and y spatial directions respectively. For the temporal discretizacion the time step has been prescribed to ∆t = 0.02. Each point of those curves corresponds to the amplitude A (distance to the laminar flow in L2-norm) of the flow (periodic or quasi-periodic) for the given value of Re. It is also marked on the curves the different stability regions, together with several Hopf bifurcations. In figure 1b at ReQ1, the Hopf bifurcation of periodic flows give rise to a family of quasi-periodic solutions, whose stability is also presented. The main load of the computations has been carried out in parallel in a Beowulf cluster of PCs.20032003-01-0120072007-05-07journal articlehttp://purl.org/coar/resource_type/c_6501NAhttp://purl.org/coar/version/c_be7fb7dd8ff6fe43info:eu-repo/semantics/articleapplication/pdfhttps://hdl.handle.net/2117/899reponame:UPCommons. Portal del coneixement obert de la UPCinstname:Universitat Politècnica de Catalunya (UPC)Inglésengopen accesshttp://purl.org/coar/access_right/c_abf2Attribution-NonCommercial-NoDerivs 2.5 Spainhttp://creativecommons.org/licenses/by-nc-nd/2.5/es/info:eu-repo/semantics/openAccessoai:upcommons.upc.edu:2117/8992026-05-27T15:37:01Z
dc.title.none.fl_str_mv Unstable manifolds computation for the two-dimensional plane Poiseuille flow
title Unstable manifolds computation for the two-dimensional plane Poiseuille flow
spellingShingle Unstable manifolds computation for the two-dimensional plane Poiseuille flow
Sánchez Casas, José Pablo
Differentiable dynamical systems
Fluid mechanics
Poiseuille flow
Unstable manifolds computation
Sistemes dinàmics diferenciables
Teoria ergòdica
Fluids
Vorticitat -- Teoria
Classificació AMS::76 Fluid mechanics::76D Incompressible viscous fluids
Classificació AMS::37 Dynamical systems and ergodic theory::37N Applications
title_short Unstable manifolds computation for the two-dimensional plane Poiseuille flow
title_full Unstable manifolds computation for the two-dimensional plane Poiseuille flow
title_fullStr Unstable manifolds computation for the two-dimensional plane Poiseuille flow
title_full_unstemmed Unstable manifolds computation for the two-dimensional plane Poiseuille flow
title_sort Unstable manifolds computation for the two-dimensional plane Poiseuille flow
dc.creator.none.fl_str_mv Sánchez Casas, José Pablo
Jorba, Angel
author Sánchez Casas, José Pablo
author_facet Sánchez Casas, José Pablo
Jorba, Angel
author_role author
author2 Jorba, Angel
author2_role author
dc.subject.none.fl_str_mv Differentiable dynamical systems
Fluid mechanics
Poiseuille flow
Unstable manifolds computation
Sistemes dinàmics diferenciables
Teoria ergòdica
Fluids
Vorticitat -- Teoria
Classificació AMS::76 Fluid mechanics::76D Incompressible viscous fluids
Classificació AMS::37 Dynamical systems and ergodic theory::37N Applications
topic Differentiable dynamical systems
Fluid mechanics
Poiseuille flow
Unstable manifolds computation
Sistemes dinàmics diferenciables
Teoria ergòdica
Fluids
Vorticitat -- Teoria
Classificació AMS::76 Fluid mechanics::76D Incompressible viscous fluids
Classificació AMS::37 Dynamical systems and ergodic theory::37N Applications
description In this work we study some aspects of the dynamics of the plane Poiseuille problem in dimension 2, in what refers to the connection among different configurations of the flow. The fluid is confined in a channel of plane parallel walls. The problem is modeled by the incompressible Navier-Stokes equations ∂u ∂t + (u · ∇)u = −∇p + 1 Re ∆u, ∇ · u = 0, (1) being Re the Reynolds number, together with no-slip on the channel walls and L-periodic boundary conditions (L = 2π/α, being α the parameter wave number). We have considered two different formulations to drive the fluid through the channel: holding constant the total flux or the mean pressure gradient. For each of them we obtain a different definition of Re = hUc/ν, where h represents half of the channel length, Uc the velocity of the laminar flow in the centre of the channel, and ν the kinematic viscosity. To be precise ReQ = 3Q/ν, Rep = Gh3ρ/2µ2, corresponds to the Reynolds numbers when we keep Q as a constant flux or G as a constant mean pressure gradient respectively. The fluid is supposed of constant density ρ and viscosity µ. The numerical approximation is detailed in [1]. Roughly, it employs Fourier and Chebyshev spectral discretizations of velocities and pressure in the periodic and transversal directions respectively. The temporal variable is approximated by means of finite differences. In figure 1 we represent bifurcating curves of periodic and quasi-periodic flows obtained numerically in [1] using N = 8 and M = 70 spectral modes in the x and y spatial directions respectively. For the temporal discretizacion the time step has been prescribed to ∆t = 0.02. Each point of those curves corresponds to the amplitude A (distance to the laminar flow in L2-norm) of the flow (periodic or quasi-periodic) for the given value of Re. It is also marked on the curves the different stability regions, together with several Hopf bifurcations. In figure 1b at ReQ1, the Hopf bifurcation of periodic flows give rise to a family of quasi-periodic solutions, whose stability is also presented. The main load of the computations has been carried out in parallel in a Beowulf cluster of PCs.
publishDate 2003
dc.date.none.fl_str_mv 2003
2003-01-01
2007
2007-05-07
dc.type.none.fl_str_mv journal article
http://purl.org/coar/resource_type/c_6501
NA
http://purl.org/coar/version/c_be7fb7dd8ff6fe43
dc.type.openaire.fl_str_mv info:eu-repo/semantics/article
format article
dc.identifier.none.fl_str_mv https://hdl.handle.net/2117/899
url https://hdl.handle.net/2117/899
dc.language.none.fl_str_mv Inglés
eng
language_invalid_str_mv Inglés
language eng
dc.rights.none.fl_str_mv open access
http://purl.org/coar/access_right/c_abf2
Attribution-NonCommercial-NoDerivs 2.5 Spain
http://creativecommons.org/licenses/by-nc-nd/2.5/es/
dc.rights.openaire.fl_str_mv info:eu-repo/semantics/openAccess
rights_invalid_str_mv open access
http://purl.org/coar/access_right/c_abf2
Attribution-NonCommercial-NoDerivs 2.5 Spain
http://creativecommons.org/licenses/by-nc-nd/2.5/es/
eu_rights_str_mv openAccess
dc.format.none.fl_str_mv application/pdf
dc.source.none.fl_str_mv reponame:UPCommons. Portal del coneixement obert de la UPC
instname:Universitat Politècnica de Catalunya (UPC)
instname_str Universitat Politècnica de Catalunya (UPC)
reponame_str UPCommons. Portal del coneixement obert de la UPC
collection UPCommons. Portal del coneixement obert de la UPC
repository.name.fl_str_mv
repository.mail.fl_str_mv
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