Numerical Investigations of Wake and Shock Wave Effects on Film Cooling Performance in a Transonic Turbine Stage, Part 1 - Methodology Development and Qualification over Stationary Stators and Rotors

To understand the unsteady shock wave and wake effects on the film cooling performance over a transonic 3-D rotating stage, a series of numerical investigations have been conducted and are presented in this two-part paper. Part 1 is focused on the development of the computational model and methodology of the system setup and model qualification; Part 2 is to investigate the unsteady effects of shock waves and wakes on film cooling performance in a transonic rotating stage. In Part 1, the film cooling experimental conditions (nonrotating) and test sections of Kopper et. al. and Hunter are selected for model qualification. The numerical computation is carried out by the commercial software Ansys/Fluent using the pressure based compressible flow governing equations. The effects of four turbulence models are carefully compared with the experimental data. The Realizable k-e turbulence model is found to match the experimental data better than the other models and is thus used for the rest of the study, including Part 2. The results show that 1) the weak shock emanating from the neighboring stator’s trailing edge results in a temperature rise and a reduction of film cooling effectiveness on the suction side near the trailing edge, 2) cooling ejection from the trailing edge reduces the shock strength in the stator passage, 3) an increase in Mach number from 0.84 to 1.50 can reduce the total pressure losses of fluid flow near the end-walls, 4) the film cooling effectiveness increases with increasing blowing ratio and becomes more even on the stator with a higher blowing ratio, and 5) an increase in Mach number from 0.84 to 1.50 gives rise to a higher cooling effectiveness in the region from the cooling holes to 80% of the chord length of the stator on the pressure side, but becomes lower after this up to the trailing edge. However, on the stator's suction side, higher Mach number results in a lower cooling effectiveness region around the film holes from 30% to 55% of the chord length, but cooling effectiveness increases downstream.

[1]  J. Larsson Turbine blade heat transfer calculations using two-equation turbulence models , 1997 .

[2]  Giovanna Barigozzi,et al.  Pressure Side and Cutback Trailing Edge Film Cooling in a Linear Nozzle Vane Cascade at Different Mach Numbers , 2012 .

[3]  T. Shih,et al.  A new k-ϵ eddy viscosity model for high reynolds number turbulent flows , 1995 .

[4]  B. Launder,et al.  Ground effects on pressure fluctuations in the atmospheric boundary layer , 1978, Journal of Fluid Mechanics.

[5]  Craig A. Hunter,et al.  Experimental, Theoretical, and Computational Investigation of Separated Nozzle Flows , 1998 .

[6]  P. Calzada,et al.  Numerical Investigation of Heat Transfer in Turbine Cascades With Separated Flows , 2003 .

[7]  Brian Launder,et al.  Second-moment closure: present… and future? , 1989 .

[8]  R. C. Stoeffler,et al.  Energy efficient engine high-pressure turbine supersonic cascade technology report , 1981 .

[9]  Wing Ng,et al.  PERFORMANCE OF A SHOWERHEAD AND SHAPED HOLE FILM COOLED VANE AT HIGH FREESTREAM TURBULENCE AND TRANSONIC CONDITIONS , 2011 .

[10]  Kwang‐Yong Kim,et al.  Shape optimization of a fan-shaped hole to enhance film-cooling effectiveness , 2010 .

[11]  F. Menter Two-equation eddy-viscosity turbulence models for engineering applications , 1994 .

[12]  B. Launder,et al.  Lectures in mathematical models of turbulence , 1972 .

[13]  A. Ameri,et al.  Numerical Analysis of Film Cooling at High Blowing Ratio , 2013 .

[14]  B. Launder,et al.  Progress in the development of a Reynolds-stress turbulence closure , 1975, Journal of Fluid Mechanics.

[15]  D. W. Bahr,et al.  Energy efficient engine , 1980 .

[16]  N. V. Nirmalan,et al.  An experimental study of turbine vane heat transfer with leading edge and downstream film cooling , 1990 .