Abstract
This report studies an abstract approach to modeling the motion of large eddies in a turbulent flow. If the Navier-Stokes equations (NSE) are averaged with a local, spatial convolution type filter, φ = g δ*φ, the resulting system is not closed due to the filtered nonlinear term uu. An approximate deconvolution operator D is a bounded linear operator which is an approximate filter inverse D(u) = approximation of u. Using this general deconvolution operator yields the closure approximation to the filtered nonlinear term in the NSE uu ∼ D(u)D(u). Averaging the Navier-Stokes equations using the above closure, possible including a time relaxation term to damp unresolved scales, yields the approximate deconvolution model (ADM) wt + ∇ D(w) D(w) - νw + ∇q + χw* = f and ∇ ̇ w = 0. Here ≃ u, χ ≥ 0, and w * is a generalized fluctuation, defined by a positive semi-definite operator. We derive conditions on the general deconvolution operator D that guarantee the existence and uniqueness of strong solutions of the model. We also derive the model's energy balance. © 2008 Università degli Studi di Ferrara.
| Original language | American English |
|---|---|
| Pages (from-to) | 145-168 |
| Number of pages | 24 |
| Journal | Annali dell'Universita' di Ferrara |
| Volume | 54 |
| Issue number | 1 |
| DOIs | |
| State | Published - May 1 2008 |
Funding
The author is partially supported by NSF grant DMS 0508260.
| Funders | Funder number |
|---|---|
| National Science Foundation | DMS 0508260 |
ASJC Scopus Subject Areas
- General Mathematics
Keywords
- Deconvolution
- Large eddy simulation
- Turbulence
Disciplines
- Mathematics
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