Axial velocity and turbulent kinetic energy, 41k to load enlargement Radial temperature profiles, 26k to load enlargement
Fig. 3: Bluff-body burner;
axial velocity and turbulence energy
Fig. 4: Bluff-body burner;
radial temperature profiles


Vortex shedding behind bluff bodies

A wide range of engineering turbulent flows feature transient phenomena which are either non-organized or periodic. The dynamics of shedding vortices in the wake of a bluff-body obstacle is perhaps the most prominent example of periodic tubulent mean flow. Apparently, it represents a very basic flow, however, the associated flow physics is far from trivial and often employed to trigger fluid engineering devices, for example, in the flame stabilazation process of a combustion chamber.

A review of recent attempts to simulate periodic turbulent flows displays a considerable disparity in their predictive capabilities. Generally, an accurate computational representation of of complex transient flows is exclusively within reach of direct numerical simulation (DNS) or large-eddy simulation (LES). Due to the extrem computational demands, the application of these structure resolving methodologies is confined to flows at low & moderate Reynolds numbers in simple geometries. Thus, simulations based on Reynolds- or phase-averaged Navier-Stokes equations in conjunction with an empirical turbulence closure model are a viable route to approach these flows for their robustnesss, geometrical flexibility and computational efficiency.

Phase-averaged streamlines, 90k to load enlargement Mean velocity and total energy distribution, 10k to load enlargement
Fig. 5: Circular cylinder at Re=500; phase-averaged
streamlines (phase 01 and 09) from DNS and RANS
Fig. 6: Mean velocity and total energy distribution on
the centre plane of the circular cylinder

The principal aim of the study is to analyze a class of recently developed efficient turbulence closure models with respect to the accuracy of flow physics representation in periodic turbulent flows. Therefore Non-linear eddy-viscosity models and explicit algebraic stress models up to cubic fragments of strain-rate and vorticity tensors are in the focal point, however the preformance of a selected realizable linear truncation is also given for completness.


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