The Navier–Stokes-alpha model of fluid turbulence
By Ciprian Foias, Darryl D. Holm, Edriss S. Titi. 2001
468 citations recorded by the source corpus.
Abstract We review the properties of the nonlinearly dispersive Navier–Stokes-alpha (NS-α) model of incompressible fluid turbulence — also called the viscous Camassa–Holm equations in the literature. We first re-derive the NS-α model by filtering the velocity of the fluid loop in Kelvin’s circulation theorem for the Navier–Stokes equations. Then we show that this filtering causes the wavenumber spectrum of the translational kinetic energy for the NS-α model to roll off as k−3 for kα>1 in three dimensions, instead of continuing along the slower Kolmogorov scaling law, k−5/3, that it follows for kα
Subfields: Applied Mathematics, Computational Mechanics
View Paper: https://www.semanticscholar.org/paper/c66ef2c69b79ca76cfed8743a96133c9588203c5
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Applied Mathematics
- Edriss S. Titi
- Darryl D. Holm
- Evelyn Lunasin
- Alexei A. Ilyin
- Bernard J. Geurts
- Y. Cao
- J. Tinsley Oden
- Jean-Luc Guermond
In Computational Mechanics
- Evelyn Lunasin
- Edriss S. Titi
- Y. Cao
- Timo Heister
- Darryl D. Holm
- Alexei A. Ilyin
- Bernard J. Geurts
- J. Löwe
Citations in the corpus
- Grad–div stabilization and subgrid pressure models for the incompressible Navier–Stokes equations (2009, background): “Note that the order of velocity and pressure finite elements was never taken into account in the considerations above.”
- Global well-posedness of the three-dimensional viscous and inviscid simplified Bardina turbulence models (2006, methodology): “We will obtain our results about the decay of the energy spectrum for the filtered velocity u following similar techniques as those in the NS-α [17].”
- Variational principles for stochastic fluid dynamics (2014, methodology): “To guarantee that the resulting stochastic partial differential equations (SPDEs) are well-posed, one may need to mollify the Lagrangian to ensure analytical control of these gradients along the lines followed for the NavierStokes-alpha turbulence models [11, 12].”
- Mathematical Perspectives on Large Eddy Simulation Models for Turbulent Flows (2004, background): “We recognize here the constitutive law of a rate-dependent incompressible homogeneous fluid of second grade in which the dissipation is slightly modified by composition with the Helmholtz operator (see [15] for more details).”
- Regularization modeling for large-eddy simulation (2002, methodology): “Of particular interest is the Lagrangian averaged NS−α model [13] which arises in the Euler-Poincaré framework for smoothed flow dynamics.”
- A modified-Leray-α subgrid scale model of turbulence (2006, methodology): “Following similar arguments to those presented in [14] and [16] (see also [3, 9, 17]) we will study in this section the energy spectra of the ML-α model.”
- On questions of decay and existence for the viscous Camassa–Holm equations (2006, unknown): “In [9], [10] these equations were studied in relation to turbulence theory, this treatment includes existence and uniqueness theorems on the torus in three dimensions.”