2. Abtract In this talk, a relatively newturbulence model named Gao-Yongturbulence model is investigated using the open source software—OpenFOAM. A newly developed statistical partial average scheme is presented. As the ensemble average is taken on two groups of turbulent fluctuations separately, the partial average scheme able to capture the first-order statistical moment of the fluctuation field, providing valuable information in addition to what have been known in the past from the conventional Reynolds average. Without any empirical coefficients, the derived equations can be used to simulate statistical mean behaviours and coherent structures of various benchmark turbulent flows. The simulated results are in good agreement with experimental data. 5/22/2009 2 Haibin_Li@hotmail.com
22. GAO-YONG TURBULENCE EUQTIONS Define the partial average of the fluctuations as: Where 5/22/2009 8 Haibin_Li@hotmail.com
23. GAO-YONG TURBULENCE EUQTIONS Applying the partial average to fluctuation equations we will get equations Model We also have continuity equation: 5/22/2009 9 Haibin_Li@hotmail.com
24. GAO-YONG TURBULENCE EUQTIONS Suppose that the constitutive relationship still exists along the direction of mean flow velocity . In coordinate system 123 constituted by , Where operator has the same meaning of “scale” in OpenFOAM Where Suppose is orthotropic and is the principal material axes Where xyz global coordinate system, is coordinate transformation tensor. 5/22/2009 10 Haibin_Li@hotmail.com
25. GAO-YONG TURBULENCE EUQTIONS energy dissipation due to eddy viscosity is the work done by fluctuation force over L also considering the phenomenon of turbulence energy inversion, item should be subtracted from the right-hand side of the second equation , therefore 5/22/2009 11 Haibin_Li@hotmail.com
42. Comparison of U-velocity profiles along a vertical line passing through the geometry centre of the cavity 5/22/2009 14 Haibin_Li@hotmail.com
43. U-velocity profiles along a vertical line passing through the geometry centre of the cavity from t=0s to t=6s, Gao-Yong turbulence model 5/22/2009 15 Haibin_Li@hotmail.com
44. U-velocity profiles along a vertical line passing through the geometry centre of the cavity from t=7s to t=80s, Gao-Yong turbulence model 5/22/2009 16 Haibin_Li@hotmail.com
45. Re=10,000 Grid 80X80X1, t=80s, Gao-Yong model by Erturk Comparison of Streamlines 5/22/2009 17 Haibin_Li@hotmail.com
46. Comparison of Streamlines Re=10,000 Grid 80X80X1, t=80s, K-Epsilon model by Erturk 5/22/2009 18 Haibin_Li@hotmail.com
50. The Stream Function Vorticity Method by Erturk Gao-Yong turbulence model t=80s Comparison of Vorticity Contour 5/22/2009 22 Haibin_Li@hotmail.com Re=10,000 Grid 80X80X1, t=80s
51. Comparison of Vorticity Contour The Stream Function Vorticity Method by Erturk K-Epsilon Turbulence model t=80s 5/22/2009 23 Haibin_Li@hotmail.com Re=10,000 Grid 80X80X1, t=80s
52.
53. Gao-Yong turbulence model is able to gain real viscosity field in complex flow under coarse grid and unsteady condition.
54. The existing closed source software has limitations to the users, and therefore fail in the research, especially in the innovation research.
55. There is an improvement space for OpenFOAM in some aspects, such as: