Bulletin of the American Physical Society
77th Annual Meeting of the Division of Fluid Dynamics
Sunday–Tuesday, November 24–26, 2024; Salt Lake City, Utah
Session C12: Interact: Turbulence
10:50 AM,
Sunday, November 24, 2024
Room: Ballroom A
Chair: Charles Meneveau, Johns Hopkins University
Abstract: C12.00018 : Mean large-scale linear response of a turbulent flow: scalar transport
Presenter:
Paolo Luchini
(University of Salerno)
Author:
Paolo Luchini
(University of Salerno)
Adding a passive scalar is particularly interesting in this respect because the basic equation of its transport (in the absence of gravitational or other feedback on the fluid's velocity) is linear by itself. For the extraction technique used here this implies that no upper bound is imposed on the amplitude of the external forcing. The problem is therefore in a sense easier than for the momentum equations. Nonetheless, the simplification is not such that a large-scale turbulent diffusion coefficient could be predicted in advance, just as it cannot for momentum, and the overall statistics of the passive scalar are known to be qualitatively similar to those of velocity. This is so much more astounding if one realizes that linearity combined with boundedness of the scalar implies that the no unstable eigenvalues can be present, whereas common wisdom places the origin of chaos in turbulence seen as a dynamical system in the combination of unstable eigenvalues, which the linearized velocity equation is known to possess, with boundedness.
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