Fluctuations in turbulent Rayleigh-Bénard convection: The role of plumes

By S. Grossmann, Detlef Lohse. 2004

282 citations recorded by the source corpus.

Subfields: Computational Mechanics, Global and Planetary Change

View Paper: https://www.semanticscholar.org/paper/cefaee0c46f1f1f7ea53d0dbe94b73c6eb2ef87e

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In Computational Mechanics

In Global and Planetary Change

Citations in the corpus

High-Reynolds number Taylor-Couette turbulence. (2016, methodology): “Therefore the unifyi g scaling t ory developed by Grossmann & Lohse (2000, 2001, 2002, 2004) for RB flow is also applicable here.”
Non-Oberbeck–Boussinesq effects in strongly turbulent Rayleigh–Bénard convection (2005, background): “Indeed, the Grossmann–Lohse unifying theory of RB convection (Grossmann & Lohse 2000, 2001, 2002, 2004), which is able to account for the measured Nu(Ra, P r) and Re(Ra, P r) in a considerable part of parameter space, employs the scaling of the Prandtl–Blasius BL theory as a central ingredient…”
Heat transfer and large scale dynamics in turbulent Rayleigh-Bénard convection (2008, methodology): “(17) As detailed by Grossmann and Lohse (2004), the kinetic and thermal BL thicknesses λu and λθ are obtained from the Prandtl-Blasius BL theory (Blasius 1 Note that the Bolgiano-Obukhov length scale does not enter here.”
Heat transport by turbulent Rayleigh–Bénard convection in cylindrical samples with aspect ratio one and larger (2005, background): “A central prediction of theoretical models of turbulent Rayleigh-Bénard convection (RBC) in a fluid heated from below [Kraichnan(1962), Siggia(1994), Kadanoff(2001), Ahlers, Grossmann & Lohse (2002), Grossmann & Lohse (2000)] is the dependence of the global heat transport on the Rayleigh number”
Torque scaling in turbulent Taylor–Couette flow between independently rotating cylinders (2007, methodology): “Quantitatively, the crossover between the lower and upper ranges has been dealt with in Grossmann & Lohse (2000, 2001, 2002); Grossmann & Lohse (2004) by substituting for the full wind amplitude U in the Nω decomposition (5.12) only the reduced wind amplitude U g(λ/δ) at the edge of the 〈ω〉A,t…”
Surface nanobubbles and nanodroplets (2015, background): “(Schlichting, 1979; Grossmann and Lohse, 2004), where Pe is the Peclet number of the flow.”
Heat transport by turbulent Rayleigh–Bénard convection in cylindrical cells with aspect ratio one and less (2004, background): “A central prediction of various theoretical models (Kraichnan 1962; Siggia 1994; Grossmann & Lohse 2000, 2001, 2002, 2004) is a relationship between N, the Rayleigh number R = αg T L3/κν (α is the isobaric thermal expension coefficient, κ the thermal diffusivity, ν the kinematic viscosity, and g…”