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Titlebook: Complex Effects in Large Eddy Simulations; Stavros C. Kassinos,Carlos A. Langer,Parviz Moin Conference proceedings 2007 Springer-Verlag Be

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Husserliana: Edmund Husserl – Materialiend adaptive mesh refinement (SAMR). A conservative flux-based approach is described. An explicit centered scheme is used in turbulent flow regions while a weighted essentially non-oscillatory (WENO) scheme is employed to capture shocks. Several two- and three-dimensional numerical experiments and val
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Husserliana: Edmund Husserl – Materialiene tube endwall. A hybrid numerical method is used that is shock capturing but which reverts to a centered scheme with low numerical viscosity in regions of smooth flow. The subgrid-scale (SGS) model is the stretched-vortex (SV) model [1].
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https://doi.org/10.1007/978-3-540-34234-2Lattice-Boltzmann methods; MHD and plasma flows; Simulation; aero-acoustics and aero-optics; calculus; co
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978-3-540-34233-5Springer-Verlag Berlin Heidelberg 2007
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Complex Effects in Large Eddy Simulations,nce. Initially limited to the simulation of turbulent flows in simple geometries, current LES tools are being applied to multidisciplinary problems involving a variety of physical processes. Several examples of recent advances in LES methodology and complex multi-physics applications are presented.
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On the Relation between Subgrid-Scale Modeling and Numerical Discretization in Large-Eddy Simulatiomation method and the subgrid-scale model are linked. One can exploit this link by developing discretization methods from subgrid-scale models, or vice versa. Approaches where SGS models and numerical discretizations are fully linked are called implicit SGS models. Different approaches to SGS modeli
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On the Investigation of a Dynamic Nonlinear Subgrid-Scale Model,the five terms are tested in a turbulent channel flow at a turbulent Reynolds number of .τ = 395. The model constants, one for each term, are determined dynamically. Some double term models showed significant improvement compared to the dynamic Smagorinsky model. Determination of two coupled dynamic
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