Instabilities in Hydrodynamics
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50:40
Numerical methods for hydrodynamic instabilities (lecture N°4) official
Numerical methods for hydrodynamic instabilities (lecture n°4)by Laurette Tuckerman (CNRS, ESPCI).Instabilities in HydrodynamicsInstitut Henri Poincaré, August 27–31 2012Symposium organized by Christophe Lacave's Emergence team and supported by the FSMP.
01:05:21
On the well-posedness of the hydrostatic limit in fluid mechanics. official
on the well-posedness of the hydrostatic limit in fluid mechanicsBy Michael Renardy (Mathematics Department, Virginia Tech)Instabilities in HydrodynamicsInstitut Henri Poincaré, August 27–31 2012Symposium organized by Christophe Lacave's Emergence team and supported by the FSMP.
01:46:15
Numerical methods for hydrodynamic instabilities (lecture n°3) official
Numerical methods for hydrodynamic instabilities (lecture n°3)by Laurette Tuckerman (CNRS, ESPCI)Instabilities in HydrodynamicsInstitut Henri Poincaré, August 27–31 2012Symposium organized by Christophe Lacave's Emergence team and supported by the FSMP.
01:06:34
Existence for the Prandtl system under the Oleinik condition official
Existence for the Prandtl system under the Oleinik conditionby Nader Masmoudi (Courant Institute of Mathematical Sciences)Instabilities in HydrodynamicsInstitut Henri Poincaré, August 27–31 2012Symposium organized by Christophe Lacave's Emergence team and supported by the FSMP.
01:04:06
Numerical methods for hydrodynamic instabilities (lecture n°2) official
Numerical methods for hydrodynamic instabilities (lecture n°2)by Laurette Tuckerman (CNRS, ESPCI)Instabilities in HydrodynamicsInstitut Henri Poincaré, August 27–31 2012Symposium organized by Christophe Lacave's Emergence team and supported by the FSMP.
02:03:59
Hydrodynamic stability and the transition to turbulence (lecture n°3) official
Hydrodynamic stability and the transition to turbulence (lecture n°3)by Paul Manneville (CNRS, Ecole Polytechnique)Instabilities in HydrodynamicsInstitut Henri Poincaré, August 27–31 2012Symposium organized by Christophe Lacave's Emergence team and supported by the FSMP.
02:05:04
Numerical methods for hydrodynamic instabilities (lecture n°1) official
Numerical methods for hydrodynamic instabilities (lecture n°1)by Laurette Tuckerman (CNRS, ESPCI)Instabilities in HydrodynamicsInstitut Henri Poincaré, August 27–31 2012Symposium organized by Christophe Lacave's Emergence team and supported by the FSMP.
01:02:09
Using non-normal transient growth for passive control official
Using non-normal transient growth for passive controlby Carlo Cossu (IMFT, CNRS & École Polytechnique)Instabilities in HydrodynamicsInstitut Henri Poincaré, August 27–31 2012Symposium organized by Christophe Lacave's Emergence team and supported by the FSMP.
02:05:37
Transverse instability of solitary waves - lecture 2 official
Transverse instability of solitary waves - lecture 2by Frédéric Rousset (Irmar, Université de Rennes 1)Instabilities in HydrodynamicsInstitut Henri Poincaré, August 27–31 2012Symposium organized by Christophe Lacave's Emergence team and supported by the FSMP.
01:09:03
The use of adjoints for stability and sensitivity analyses official
The use of adjoints for stability and sensitivity analysesby Peter Schmid (LadHyX, École Polytechnique)Instabilities in HydrodynamicsInstitut Henri Poincaré, August 27–31 2012Symposium organized by Christophe Lacave's Emergence team and supported by the FSMP.
57:46
High Reynolds number limit for Navier Stokes equations official
High Reynolds number limit for Navier Stokes equationsby Emmanuel Grenier (UMPA, ENS Lyon & Numed, Inria)Instabilities in HydrodynamicsInstitut Henri Poincaré, August 27–31 2012Symposium organized by Christophe Lacave's Emergence team and supported by the FSMP.
02:06:26
Hydrodynamic stability and the transition to turbulence (lecture 2) official
Hydrodynamic stability and the transition to turbulence (lecture 2)by Paul Manneville (CNRS, Ecole Polytechnique)Instabilities in HydrodynamicsInstitut Henri Poincaré, August 27–31 2012Symposium organized by Christophe Lacave's Emergence team and supported by the FSMP.
01:07:53
Current Hole instability and reduced resistive MH models in Tokamaks official
Current Hole instability and reduced resistive MH models in Tokamaksby Bruno Després (Laboratoire J.-L. Lions, UPMC)Instabilities in HydrodynamicsInstitut Henri Poincaré, August 27–31 2012Symposium organized by Christophe Lacave's Emergence team and supported by the FSMP.
02:04:07
Transverse instability of solitary waves - lecture 1 official
Transverse instability of solitary waves - lecture 1by Frédéric Rousset (Irmar, Université de Rennes 1)Instabilities in HydrodynamicsInstitut Henri Poincaré, August 27–31 2012Symposium organized by Christophe Lacave's Emergence team and supported by the FSMP.
01:11:00
Inviscid limit for the Navier-Stokes equation with free surface official
Inviscid limit for the Navier-Stokes equation with free surfaceby Frédéric Rousset (Irmar, Université de Rennes 1)Instabilities in HydrodynamicsInstitut Henri Poincaré, August 27–31 2012Symposium organized by Christophe Lacave's Emergence team and supported by the FSMP.
43:56
On the stability of the Jeffery-Hamel problem official
On the stability of the Jeffery-Hamel problemby Julien Guillod (Université de Genève)Instabilities in HydrodynamicsInstitut Henri Poincaré, August 27–31 2012Symposium organized by Christophe Lacave's Emergence team and supported by the FSMP.
44:15
Persistence of geometric structures for inviscid incompressible fluids official
Persistence of geometric structures for inviscid incompressible fluidsby Francesco Fanelli (Université Paris-Est)Instabilities in HydrodynamicsInstitut Henri Poincaré, August 27–31 2012Symposium organized by Christophe Lacave's Emergence team and supported by the FSMP.
02:02:13
Hydrodynamic stability and the transition to turbulence official
Hydrodynamic stability and the transition to turbulenceby Paul Manneville (CNRS, Ecole Polytechnique)Instabilities in HydrodynamicsInstitut Henri Poincaré, August 27–31 2012Symposium organized by Christophe Lacave's Emergence team and supported by the FSMP.