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I.K. Marchevsky, V.V. Puzikova

32

ISSN 1812-3368. Вестник МГТУ им. Н.Э. Баумана. Сер. Естественные науки. 2017. № 5

Flow simulation at high Reynolds numbers

5

7

(Re =10 10 ).

The flow was

simulated at the Reynolds numbers

5

7

Re =10 10

(on non-uniform meshes

240 296

with

4

= 5 10

t

 

and 480 592

with

4

=10

t

). Results obtained on mesh

480 592

are very close to experimental data [18], see Fig. 6. At

5

Re = 2 10 ,

the

boundary layer on the cylinder surface undergoes a transition from laminar to

turbulent [19]. This transition leads to a delay of the separation of flow from the

cylinder surface causing a substantial reduction in the drag force. This is often

referred to as ''drag crisis''. This phenomenon was simulated by using modified

LS-STAG immersed boundary method (Fig. 6).

Conclusions.

The key points of the LS-STAG method [2, 21] extension for

RANS/LES/DES turbulence models were described. For the shear Reynolds stresses

and for the eddy viscosity an additional mesh (

xy

-mesh) is introduced. The general

approach to the construction of the LS-STAG discretization for differential equations

of the EVM models on the additional

xy

-mesh shown. The Smagorinsky, Spalart —

Allmaras,

,

k

 

k



and

k



SST turbulence models are considered. To validate

modified LS-STAG immersed boundary method the flow past a circular airfoil at

2

7

Re =10 10

was simulated. Computational results are in good agreement with

established results from the literature. Also, the so-called ''drag crisis'' phenomenon of

circular cylinder at

5

6

Re =10 10

was simulated.

REFERENCES

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