Bulk flow pulsations and film cooling : Flow structure just downstream of the holes

Experimental results are presented that describe the effects of bulk flow pulsations on film cooling from a single row of simple angle film cooling holes. The pulsations are in the form of sinusoidal variations of static pressure and streamwise velocity. Such pulsations are important in turbine studies because: (i) Static pressure pulsations result in significant periodic variations of film cooling flow rates, coverage, and trajectories, and (ii) static pressure pulsations occur near blade surfaces in operating engines from potential flow interactions between moving blade rows and from families ofpassing shock waves. Distributions of ensemble-averaged and time-averaged Reynolds stress tensor components are investigated just downstream of the holes along with distributions of all three mean velocity components. Important changes are evident in all measured quantities. In particular, maximum Reynolds shear stresses -2u'v'/u∞ 2 are lower in regions containing the largest film concentrations because the strong shear layer produced by the injectant is more three dimensional, larger in extent, and oscillates its position from the wall with time.

[1]  R. P. Dring,et al.  An Experimental Investigation of Film Cooling on a Turbine Rotor Blade , 1980 .

[2]  C. P. Lee,et al.  Unsteady Wake Over a Linear Turbine Blade Cascade With Air and CO2 Film Injection: Part II—Effect on Film Effectiveness and Heat Transfer Distributions , 1994 .

[3]  Roger W. Ainsworth,et al.  Surface Heat Transfer Fluctuations on a Turbine Rotor Blade Due to Upstream Shock Wave Passing , 1989 .

[4]  Denis J. Doorly,et al.  Simulation of the Effects of Shock Wave Passing on a Turbine Rotor Blade , 1985 .

[5]  A. Hussain,et al.  The mechanics of an organized wave in turbulent shear flow , 1970, Journal of Fluid Mechanics.

[6]  B. Ramaprian,et al.  Experimental study of a periodic turbulent boundary layer in zero mean pressure gradient , 1989, The Aeronautical Journal (1968).

[7]  M. L. G. Oldfield,et al.  Gas Turbine Rotor Blade Film Cooling With and Without Simulated NGV Shock Waves and Wakes , 1990 .

[8]  Je-Chin Han,et al.  Unsteady Wake Effect on Film Effectiveness and Heat Transfer Coefficient From a Turbine Blade With One Row of Air and CO2 Film Injection , 1994 .

[9]  Reza S. Abhari,et al.  An Experimental Study of Film Cooling in a Rotating Transonic Turbine , 1994 .

[10]  C. P. Lee,et al.  Unsteady Wake Over a Linear Turbine Blade Cascade With Air and CO2 Film Injection: Part I — Effect on Heat Transfer Coefficients , 1993 .

[11]  Robert J. Moffat,et al.  Describing the Uncertainties in Experimental Results , 1988 .

[12]  S. Aoki,et al.  Film Cooling on a Gas Turbine Rotor Blade , 1991 .

[13]  Sture K. F. Karlsson,et al.  An unsteady turbulent boundary layer , 1959, Journal of Fluid Mechanics.

[14]  P. S. Klebanoff,et al.  Characteristics of turbulence in a boundary layer with zero pressure gradient , 1955 .

[15]  K. Al-Asmi,et al.  Production of oscillatory flow in wind tunnels , 1993 .

[16]  B. R. Ramaprian,et al.  An experimental study of oscillatory pipe flow at transitional Reynolds numbers , 1980, Journal of Fluid Mechanics.

[17]  D. L. Schultz,et al.  Unsteady Aerodynamic and Heat Transfer Processes in a Transonic Turbine Stage , 1985 .

[18]  R. S. Abhari,et al.  Comparison of Time-Resolved Turbine Rotor Blade Heat Transfer Measurements and Numerical Calculations , 1992 .

[19]  Phillip M. Ligrani,et al.  Bulk Flow Pulsations and Film Cooling: Flow Structure Just Downstream of the Holes , 1995 .

[20]  Phillip M. Ligrani,et al.  Film-Cooling From Holes With Compound Angle Orientations: Part 1—Results Downstream of Two Staggered Rows of Holes With 3d Spanwise Spacing , 1994 .