theorem A.767 Marginal stability of the conducting state

open in the book · appendices/A-long-proofs.tex:37349 · p. 3168

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theorem A.767: Marginal stability of the conducting stateA.767phenomenon 31.78: Convective onset at a computed threshold31.78proposition A.766: NondimensionalisationA.766remark A.768: Two conventions for the wavenumberA.768theorem A.769: The Lorenz systemA.769proof : app:A-long-proofs@proof-446proofdefinition 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 costs31.81proof : ch:14-fluid-dynamics@proof-39proofproposition A.765: The roll equationsA.765proof : app:A-long-proofs@proof-445proofequation 31.68: eq:fluid-racrit31.68definition 32.62: The Lorenz system32.62remark A.771: What was assumed, and where it failsA.771remark A.770: What the three variables and three parameters areA.770proof : app:A-long-proofs@proof-447proof

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typedirectionnode provenancewhere
depends_on Convective onset at a computed threshold declared appendices/A-long-proofs.tex:37369
depends_on Nondimensionalisation declared appendices/A-long-proofs.tex:37369
depends_on Two conventions for the wavenumber declared appendices/A-long-proofs.tex:37442
depends_on The Lorenz system declared appendices/A-long-proofs.tex:37487
proves app:A-long-proofs@proof-446 declared appendices/A-long-proofs.tex:37372