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In fluid dynamics and turbulence theory, Reynolds decomposition is a mathematical technique used to separate the expectation value of a quantity from its fluctuations.
Decomposition
For example, for a quantity the decomposition would be
The expected value, , is often found from an ensemble average which is an average taken over multiple experiments under identical conditions. The expected value is also sometime denoted , but it is also seen often with the over-bar notation.[3]
Direct numerical simulation, or resolution of the Navier–Stokes equations completely in , is only possible on extremely fine computational grids and small time steps even when Reynolds numbers are low, and becomes prohibitively computationally expensive at high Reynolds' numbers. Due to computational constraints, simplifications of the Navier-Stokes equations are useful to parameterize turbulence that are smaller than the computational grid, allowing larger computational domains.[4]
Reynolds decomposition allows the simplification of the Navier–Stokes equations by substituting in the sum of the steady component and perturbations to the velocity profile and taking the mean value. The resulting equation contains a nonlinear term known as the Reynolds stresses which gives rise to turbulence.
See also
References
- ^ Müller, Peter (2006). The Equations of Oceanic Motions. p. 112.
- ^ Adrian, R (2000). "Analysis and Interpretation of instantaneous turbulent velocity fields". Experiments in Fluids. 29 (3): 275–290. Bibcode:2000ExFl...29..275A. doi:10.1007/s003489900087. S2CID 122145330.
- ^ Kundu, Pijush (27 March 2015). Fluid Mechanics. Academic Press. p. 609. ISBN 978-0-12-405935-1.
- ^ Mukerji, Sudip (1997). Turbulence Computations with 3-D Small-Scale Additive Turbulent Decomposition and Data-Fitting Using Chaotic Map Combinations (PhD thesis). University of Kentucky. doi:10.2172/666048. OSTI 666048. ProQuest 304354392.
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