Effect of Mach Number on Secondary Flow Characteristics

Endwall secondary f lows in gas turbines are complicated by highly non-uniform combustor exit profiles. Most experimental endwall studies do match turbine Reynolds numbers, but not Mach numbers, and assume constant temperature conditions with a simple turbulent boundary layer. This paper presents results for benchmarking of a CFD code with experimental data and the effects of inlet profiles at both low and high Mach number conditions under matched Reynolds number conditions. Detailed flowfield measurements were obtained in a large scale, linear turbine vane cascade and were used for CFD benchmarking. Analysis of the results for spanwise varying inlet profiles indicate that the stagnation pressure gradient is the key parameter in determining the character of the secondary f lows in the first Stator vane passage. Temperature gradients applied at the inlet were distorted in relation to the secondary f lows influencing heat transfer to the vane and the inlet thermal field for the next rotor stage. Comparisons of CFD simulations at engine operating Mach number and Reynolds number conditions to the low-speed wind tunnel simulations indicate that the secondary flow pattern develops similarly up to the location of the shock.

[1]  H. G. Loos Compressibility effects on secondary flows , 1956 .

[2]  W. J. Whitney,et al.  Performance of a high-work low aspect ratio turbine tested with a realistic inlet radial temperature profile , 1984 .

[3]  B. Lakshminarayana,et al.  Effects of Inlet Temperature Gradients on Turbomachinery Performance , 1975 .

[4]  Roger L. Davis,et al.  Unsteady analysis of hot streak migration in a turbine stage , 1990 .

[5]  B. Launder,et al.  The numerical computation of turbulent flows , 1990 .

[6]  Clifford E. Smith,et al.  CFD Modeling of a Gas Turbine Combustor From Compressor Exit to Turbine Inlet , 1999 .

[7]  Robert P. Dring,et al.  Navier-Stokes analyses of the redistribution of inlet temperature distortions in a turbine , 1990 .

[8]  Antonio Giovanni Perdichizzi Mach Number Effects on Secondary Flow Development Downstream of a Turbine Cascade , 1990 .

[9]  Karen A. Thole,et al.  Effect of inlet conditions on endwall secondary flows , 1999 .

[10]  S. Orszag,et al.  Development of turbulence models for shear flows by a double expansion technique , 1992 .

[11]  L. S. Langston,et al.  Crossflows in a Turbine Cascade Passage , 1980 .

[12]  D. G. Gregory-Smith,et al.  Growth of Secondary Losses and Vorticity in an Axial Turbine Cascade , 1988 .

[13]  Om P. Sharma,et al.  Predictions of Endwall Losses and Secondary Flows in Axial Flow Turbine Cascades , 1986 .

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

[15]  Karen A. Thole,et al.  Heat Transfer and Flowfield Measurements in the Leading Edge Region of a Stator Vane Endwall , 1999 .

[16]  R. J. Boyle,et al.  Prediction of Nonuniform Inlet Temperature Effects on Vane and Rotor Heat Transfer , 1997 .

[17]  H. D. Joslyn,et al.  Redistribution of an inlet temperature distortion in an axial flow turbine stage , 1989 .

[18]  W. Hawthorne,et al.  Secondary circulation in fluid flow , 1951, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[19]  M. F. Blair,et al.  An Experimental Study of Endwall and Airfoil Surface Heat Transfer in a Large Scale Turbine Blade Cascade , 1980 .

[20]  C. H. Sieverding,et al.  Influence of Mach Number and End Wall Cooling on Secondary Flows in a Straight Nozzle Cascade , 1981 .

[21]  Karen A. Thole,et al.  Flowfield Measurements in the Endwall Region of a Stator Vane , 1999 .