An investigation of the heat transfer and static pressure on the over-tip casing wall of an axial turbine operating at engine representative flow conditions. (II). Time-resolved results

Abstract The over-tip casing of the high-pressure turbine in a modern gas turbine engine is subjected to strong convective heat transfer that can lead to thermally induced failure (burnout) of this component. However, the complicated flow physics in this region is dominated by the close proximity of the moving turbine blades, which gives rise to significant temporal variations at the blade-passing frequency. The understanding of the physical processes that control the casing metal temperature is still limited and this fact has significant implications for the turbine design strategy. A series of experiments has been performed that seeks to address some of these important issues. This article reports the measurements of time-mean heat transfer and time-mean static pressure that have been made on the over-tip casing of a transonic axial-flow turbine operating at flow conditions that are representative of those found in modern gas turbine engines. Time-resolved measurements of these flow variables (that reveal the details of the blade-tip/casing interaction physics) are presented in a companion paper. The nozzle guide vane exit flow conditions in these experiments were a Mach number of 0.93 and a Reynolds number of 2.7 × 10 6 based on nozzle guide vane mid-height axial chord. The axial and circumferential distributions of heat transfer rate, adiabatic wall temperature, Nusselt number and static pressure are presented. The data reveal large axial variations in the wall heat flux and adiabatic wall temperature that are shown to be primarily associated with the reduction in flow stagnation temperature through the blade row. The heat flux falls by a factor of 6 (from 120 to 20 kW/m 2 ). In contrast, the Nusselt number falls by just 36% between the rotor inlet plane and 80% rotor axial chord; additionally, this drop is near to linear from 20% to 80% rotor axial chord. The circumferential variations in heat transfer rate are small, implying that the nozzle guide vanes do not produce a strong variation in casing boundary layer properties in the region measured. The casing static pressure measurements follow trends that can be expected from the blade loading distribution, with maximum values immediately upstream of the rotor inlet plane, and then a decreasing trend with axial position as the flow is turned and accelerated in the relative frame of reference. The time-mean static pressure measurements on the casing wall also reveal distinct circumferential variations that are small in comparison to the large pressure gradient in the axial direction.

[1]  T. V. Jones,et al.  Heat-transfer measurements in short-duration hypersonic facilities , 1973 .

[2]  H. Schlichting Boundary Layer Theory , 1955 .

[3]  Roger W. Ainsworth,et al.  Unsteady Pressure Measurement , 2000 .

[4]  Tony Arts,et al.  Aero-Thermal Performance of a Two-Dimensional Highly Loaded Transonic Turbine Nozzle Guide Vane: A Test Case for Inviscid and Viscous Flow Computations , 1992 .

[5]  Anthony G. Sheard,et al.  A Transient Flow Facility for the Study of the Thermofluid-Dynamics of a Full Stage Turbine Under Engine Representative Conditions , 1988 .

[6]  W. G. Steele,et al.  Engineering application of experimental uncertainty analysis , 1995 .

[7]  Richard J Goldstein,et al.  Effects of Tip Geometry and Tip Clearance on the Mass/Heat Transfer From a Large-Scale Gas Turbine Blade , 2003 .

[8]  F. Martelli,et al.  Investigation of the Unsteady Rotor Aerodynamics in a Transonic Turbine Stage , 2001 .

[9]  J. P. Bindon,et al.  The Effect of Tip Clearance on the Development of Loss Behind a Rotor and a Subsequent Nozzle , 1997 .

[10]  Neil William Harvey,et al.  Wake, Shock, and Potential Field Interactions in a 1.5 Stage Turbine—Part I: Vane-Rotor and Rotor-Vane Interaction , 2003 .

[11]  Howard P. Hodson,et al.  The Effect of Blade Tip Geometry on the Tip Leakage Flow in Axial Turbine Cascades , 1991 .

[12]  D. E. Metzger,et al.  Heat Transfer and Effectiveness on Film Cooled Turbine Blade Tip Models , 1995 .

[13]  Richard J Goldstein,et al.  Effect of Endwall Motion on Blade Tip Heat Transfer , 2003 .

[14]  J. P. Bindon,et al.  The measurement and formation of tip clearance loss , 1989 .

[15]  D. E. Metzger,et al.  The Influence of Turbine Clearance Gap Leakage on Passage Velocity and Heat Transfer Near Blade Tips: Part II—Source Flow Effects on Blade Suction Sides , 1989 .

[16]  A. Yamamoto,et al.  Endwall Flow/Loss Mechanisms in a Linear Turbine Cascade With Blade Tip Clearance , 1989 .

[17]  Alan H. Epstein,et al.  TIME RESOLVED MEASUREi.lENTS OF A TURBINE IROTUR STATIONARY TIP CASING PRESSURE AND HEAT Tt?AN!IFER FIELD , 1985 .

[18]  Roger W. Ainsworth,et al.  Heat Transfer to Rotating Turbine Blades in a Flow Undisturbed by Wakes , 1994 .

[19]  J. G. Moore,et al.  Flow and Heat Transfer in Turbine Tip Gaps , 1989 .

[20]  A. J. Dietz,et al.  Unsteady Pressure Measurements on the Rotor of a Model Turbine Stage in a Transient Flow Facility , 1992 .

[21]  Gary D. Lock,et al.  Endwall heat transfer measurements in an annular cascade of nozzle guide vanes at engine representative Reynolds and Mach numbers , 1996 .

[22]  Michael G. Dunn,et al.  Turbine Tip and Shroud Heat Transfer , 1991 .

[23]  Roger W. Ainsworth,et al.  Developments in Instrumentation and Processing for Transient Heat Transfer Measurement in a Full-Stage Model Turbine , 1989 .

[24]  R S Bunker,et al.  A Review of Turbine Blade Tip Heat Transfer , 2001, Annals of the New York Academy of Sciences.

[25]  G. W. Meetham Use of protective coatings in aero gas turbine engines , 1986 .