phenomenon 31.78 Convective onset at a computed threshold

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phenomenon 31.78: Convective onset at a computed threshold31.78definition 31.51: The other similarity groups31.51theorem 31.37: The Navier–Stokes equations31.37proposition A.761: The Boussinesq equationsA.761remark 31.79: Bénard's own cells, and Taylor's cylinders31.79remark 31.81: Where the threshold comes from, and what it costs31.81theorem A.767: Marginal stability of the conducting stateA.767proof : ch:14-fluid-dynamics@proof-39proofphenomenon 31.49: Dynamical similarity31.49theorem D.2: Buckingham's \Pi theoremD.2definition A.760: The convecting layerA.760proposition A.766: NondimensionalisationA.766remark 31.89: The Mach number and the regimes it separates31.89theorem 31.36: The Newtonian constitutive relation31.36theorem 31.22: Euler's equations of motion31.22definition A.741: The statistical settingA.741definition 31.43: Creeping flow31.43phenomenon 31.41: The fourth-power law of pipe flow31.41proposition 31.40: Circular Couette flow31.40proposition 31.39: Plane Couette flow31.39remark 31.48: What is actually proved31.48remark 31.38: Whose equations, and the Stokes hypothesis31.38theorem A.745: Kármán–Howarth–Monin relationA.745theorem 31.71: Boundary-layer thickness31.71theorem 31.82: The Reynolds-averaged equations31.82theorem 31.58: The vorticity transport equation31.58proof : ch:14-fluid-dynamics@proof-18proofdefinition A.763: Two-dimensional rollsA.763proposition A.765: The roll equationsA.765proof : app:A-long-proofs@proof-443proofproposition 31.80: Rayleigh's circulation criterion31.80remark A.768: Two conventions for the wavenumberA.768theorem A.769: The Lorenz systemA.769proof : app:A-long-proofs@proof-446proof

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cites (evidence) Étude expérimentale des courants de convection dans une nappe liquide. --- Régime permanent : tourbillons cellulaires derived parts/03-classical-mechanics/14-fluid-dynamics.tex:2594
cites (context) Hydrodynamic and Hydromagnetic Stability derived parts/03-classical-mechanics/14-fluid-dynamics.tex:2606
cites On convection currents in a horizontal layer of fluid, when the higher temperature is on the under side derived parts/03-classical-mechanics/14-fluid-dynamics.tex:2597
depends_on The other similarity groups declared parts/03-classical-mechanics/14-fluid-dynamics.tex:2608
depends_on The Navier–Stokes equations declared parts/03-classical-mechanics/14-fluid-dynamics.tex:2608
depends_on The Boussinesq equations declared appendices/A-long-proofs.tex:37111
depends_on Bénard's own cells, and Taylor's cylinders declared parts/03-classical-mechanics/14-fluid-dynamics.tex:2658
depends_on Where the threshold comes from, and what it costs declared parts/03-classical-mechanics/14-fluid-dynamics.tex:2754
depends_on Marginal stability of the conducting state declared appendices/A-long-proofs.tex:37369
proves ch:14-fluid-dynamics@proof-39 declared parts/03-classical-mechanics/14-fluid-dynamics.tex:2611