2009
DOI: 10.1140/epjb/e2009-00196-1
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Dynamical and thermodynamical stability of two-dimensional flows: variational principles and relaxation equations

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Cited by 46 publications
(139 citation statements)
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“…We note that the critical points of these different maximization problems (microcanonical, canonical, and grand canonical) are all given by Equation (229). However, the stability of the solutions (whether they are true maxima or saddle points of the thermodynamical potential) may differ because the ensembles can be inequivalent [84,89]. In [89], we have introduced different types of relaxation equations associated with these maximization problems.…”
Section: Application To 2d Turbulencementioning
confidence: 99%
See 3 more Smart Citations
“…We note that the critical points of these different maximization problems (microcanonical, canonical, and grand canonical) are all given by Equation (229). However, the stability of the solutions (whether they are true maxima or saddle points of the thermodynamical potential) may differ because the ensembles can be inequivalent [84,89]. In [89], we have introduced different types of relaxation equations associated with these maximization problems.…”
Section: Application To 2d Turbulencementioning
confidence: 99%
“…However, the stability of the solutions (whether they are true maxima or saddle points of the thermodynamical potential) may differ because the ensembles can be inequivalent [84,89]. In [89], we have introduced different types of relaxation equations associated with these maximization problems. Although being phenomenological, these equations may describe the dynamical evolution of the system towards equilibrium.…”
Section: Application To 2d Turbulencementioning
confidence: 99%
See 2 more Smart Citations
“…Thus, for β > γ + 1 , δ 2 J [q 1 , q 2 ] < 0 for every perturbation (δq 1 , δq 2 ). This is the condition of grand-canonical stability, which implies in particular microcanonical stability [49].…”
Section: A Grand-canonical Stabilitymentioning
confidence: 99%