theorem 31.82 The Reynolds-averaged equations

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theorem 31.82: The Reynolds-averaged equations31.82theorem 31.37: The Navier–Stokes equations31.37remark 31.83: The closure problem, stated exactly31.83proof : ch:14-fluid-dynamics@proof-41prooftheorem 31.36: The Newtonian constitutive relation31.36theorem 31.22: Euler's equations of motion31.22definition A.741: The statistical settingA.741definition A.760: The convecting layerA.760definition 31.43: Creeping flow31.43phenomenon 31.78: Convective onset at a computed threshold31.78phenomenon 31.41: The fourth-power law of pipe flow31.41phenomenon 31.49: Dynamical similarity31.49proposition A.761: The Boussinesq equationsA.761proposition 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 31.58: The vorticity transport equation31.58proof : ch:14-fluid-dynamics@proof-18proofremark 31.87: What a theory of turbulence would have to do31.87

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typedirectionnode provenancewhere
cites On the dynamical theory of incompressible viscous fluids and the determination of the criterion derived parts/03-classical-mechanics/14-fluid-dynamics.tex:2787
depends_on The Navier–Stokes equations declared parts/03-classical-mechanics/14-fluid-dynamics.tex:2788
depends_on The closure problem, stated exactly declared parts/03-classical-mechanics/14-fluid-dynamics.tex:2837
proves ch:14-fluid-dynamics@proof-41 declared parts/03-classical-mechanics/14-fluid-dynamics.tex:2791