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
[1] Mittal R., Iaccarino G. Immersed boundary methods.
Ann. Rev. Fluid Mech.
, 2005, vol. 37,
pp. 239–261. DOI: 10.1146/annurev.fluid.37.061903.175743
Available at:
http://www.annualreviews.org/doi/abs/10.1146/annurev.fluid.37.061903.175743[2] Cheny Y., Botella O. The LS-STAG method: A new immersed boundary/level-set method for
the computation of incompressible viscous flows in complex moving geometries with good
conservation properties.
J. Comput. Phys.
, 2010, vol. 229, iss. 4, pp. 1043–1076.
DOI: 10.1016/j.jcp.2009.10.007
[3]
Spalart P.R. Strategies for turbulence modelling and simulations.
Int. J. Heat and Fluid Flow
.
2000, vol. 21, iss. 3, pp. 252–263. DOI: 10.1016/S0142-727X(00)00007-2
[4]
Spalart P.R., Allmaras S.R. A one-equation turbulence model for aerodynamic flows.
Recherche
Aerospatiale
, 1994, no. 1, pp. 5–21.
[5]
Jones W.P., Launder B.E. The prediction of laminarization with a two-equation model of
turbulence.
Int. J. Heat Mass Transfer
, 1972, vol. 15, iss. 2, pp. 301–314.
DOI: 10.1016/0017-9310(72)90076-2
[6] Wilcox D.C. Reassessment of the scale-determining equation for advanced turbulence models.
AIAA Journal
, 1988, vol. 26, no. 11, pp. 1299–1310. DOI: 10.2514/3.10041
Available at:
https://arc.aiaa.org/doi/abs/10.2514/3.10041?journalCode=aiaaj[7] Menter F.R. Two-equation eddy-viscosity turbulence models for engineering applications.
AIAA Journal
, 1994, vol. 32, no. 8, pp. 1598–1605. DOI: 10.2514/3.12149
Available at:
https://arc.aiaa.org/doi/abs/10.2514/3.12149?journalCode=aiaaj