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Rapid distortion theory and the ‘problems’ of turbulence
318
Citations
71
References
1990
Year
The paper classifies problems in analyzing turbulent flows, noting that turbulent structure depends on domain scale, boundary geometry, and boundary condition information. The study reviews recent RDT developments and examines how RDT helps explain persistent eddy features and general turbulent flow characteristics near boundaries in slowly changing turbulent flows. Rapid distortion theory (RDT) is a linear analysis method for rapidly changing turbulent flows under distortions such as velocity gradients, bounding surfaces, and body forces; the authors apply recent RDT developments, including validity criteria and solutions incorporating inhomogeneities and boundaries, to analyze energy spectra in shear flows at moderate Reynolds numbers. RDT predicts that slowly varying turbulent features are governed by particular solutions that are insensitive to the initial energy spectrum and anisotropy, and that in moderate‑Reynolds shear flows the spectrum tends toward a k⁻² scaling over a growing portion of the spectrum due to shear, regardless of the initial spectrum.
The ‘problems’ associated with analysing different kinds of turbulent flow and different methods of solution are classified and discussed with reference to how the turbulent structure in a flow domain depends on the scale and geometry of the domain's boundary, and on the information provided in the boundary conditions. Rapid distortion theory (RDT) is a method, based on linear analysis, for calculating ‘rapidly changing turbulent’ (RCT) flows under the action of different kinds of distortion, such as large-scale velocity gradients, the effects of bounding surfaces, body forces, etc. Recent developments of the theory are reviewed, including the criteria for its validity, and new solutions allowing for the effects of inhomogeneities and boundaries.We then consider the contribution of RDT to understanding the fundamental problems of ‘slowly changing turbulent’ (SCT) flows, such as why are similar and persistent features of the local eddy structure found in different kinds of shear flow, and what are the general features of turbulent flows near boundaries. These features, which can be defined in terms of certain statistical quantities and flow patterns in individual flow realizations, are found to correspond to the form of particular solutions of RDT which change slowly over the time of the distortion. The most general, features are insensitive to the energy spectrum and to the initial anisotropy of the turbulence. A new RDT analysis of the energy spectra E(k) indicates why, in shear flows at moderate Reynolds number, the turbulence tends to have similar forms of spectra for eddies on a local scale, despite the Reynolds number not being large enough for the existence of a nonlinear cascade and there being no universal forms of spectra for unsheared turbulence; for this situation, the action of shear dU1/dx2 changes the form of the spectrum, so that, as β = (tdU1/dx2 increases, over an increasing part of the spectrum defined in terms of the integral scale L by β−1 [Gt ] kL, E(k) ∝ k−2, whatever the form of initial spectrum of E0(k) (provided E(k) = o(k−2) for kL [Gt ] 1).
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