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Existence theory of abstract approximate deconvolution models of turbulence
Authors:Iuliana Stanculescu
Affiliation:(1) Department of Mathematics, University of Pittsburgh, Pittsburgh, PA 15260, USA
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, $$overline{bf phi} = g_{delta},*,{bf phi}$$ , the resulting system is not closed due to the filtered nonlinear term $$overline{bf uu}$$ . An approximate deconvolution operator D is a bounded linear operator which is an approximate filter inverse
$$D(overline{bf u}) = {rm approximation,of}, {bf u}.$$
Using this general deconvolution operator yields the closure approximation to the filtered nonlinear term in the NSE
$$overline{bf uu} simeq overline{D(overline{bf u})D(overline{bf u})}.$$
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)
$${bf w}_{t} + nabla cdot overline{D({bf w}),D({bf w})} - nu triangle{bf w}+nabla q + chi {bf w}^* = overline{bf f} quad {rm and} quad nabla cdot {bf w} = 0.$$
Here $${bf w} simeq overline{bf u}$$ , 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. The author is partially supported by NSF grant DMS 0508260.
Keywords:Large eddy simulation  Turbulence  Deconvolution
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