proposition A.766 Nondimensionalisation

open in the book · appendices/A-long-proofs.tex:37259 · p. 3167

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proposition A.766: NondimensionalisationA.766definition 31.51: The other similarity groups31.51proposition A.765: The roll equationsA.765theorem A.767: Marginal stability of the conducting stateA.767theorem A.769: The Lorenz systemA.769proof : app:A-long-proofs@proof-445proofphenomenon 31.49: Dynamical similarity31.49theorem D.2: Buckingham's \Pi theoremD.2definition A.760: The convecting layerA.760phenomenon 31.78: Convective onset at a computed threshold31.78remark 31.89: The Mach number and the regimes it separates31.89definition A.763: Two-dimensional rollsA.763proposition A.761: The Boussinesq equationsA.761proof : app:A-long-proofs@proof-444proofremark A.768: Two conventions for the wavenumberA.768proof : app:A-long-proofs@proof-446proofdefinition 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 The other similarity groups declared appendices/A-long-proofs.tex:37289
depends_on The roll equations declared appendices/A-long-proofs.tex:37289
depends_on Marginal stability of the conducting state declared appendices/A-long-proofs.tex:37369
depends_on The Lorenz system declared appendices/A-long-proofs.tex:37487
proves app:A-long-proofs@proof-445 declared appendices/A-long-proofs.tex:37292