remark 31.79 Bénard's own cells, and Taylor's cylinders

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remark 31.79: Bénard's own cells, and Taylor's cylinders31.79phenomenon 31.78: Convective onset at a computed threshold31.78proposition 31.40: Circular Couette flow31.40definition 31.51: The other similarity groups31.51theorem 31.37: The Navier–Stokes equations31.37proposition A.761: The Boussinesq equationsA.761remark 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-39proofproposition 31.39: Plane Couette flow31.39proposition 31.80: Rayleigh's circulation criterion31.80proof : ch:14-fluid-dynamics@proof-20proof

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typedirectionnode provenancewhere
cites (context) Hydrodynamic and Hydromagnetic Stability derived parts/03-classical-mechanics/14-fluid-dynamics.tex:2655
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:2656
cites (evidence) Stability of a viscous liquid contained between two rotating cylinders derived parts/03-classical-mechanics/14-fluid-dynamics.tex:2651
depends_on Convective onset at a computed threshold declared parts/03-classical-mechanics/14-fluid-dynamics.tex:2658
depends_on Circular Couette flow declared parts/03-classical-mechanics/14-fluid-dynamics.tex:2658