Averaged and Time-Dependent Aerodynamics of a High Pressure Turbine Blade Tip Cavity and Stationary Shroud: Comparison of Computational and Experimental Results
Abstract:The unsteady aero-dynamics of a single-stage high-pressure turbine blade operating at design corrected conditions has been the subject of a thorough study involving detailed measurements and computations. The experimental configuration consisted of a single-stage high-pressure turbine and the adjacent, downstream, low-pressure turbine nozzle row. All three blade-rows were instrumented at three spanwise locations with flush-mounted, high-frequency response pressure transducers. The rotor was also instrumented w… Show more
“…Secondly the effectiveness of the tip treatments seems to lack a consistent and conclusive trend, given the relatively large amount of efforts already made on the relatively small suction side Mach number near or above the sonic condition has also been pointed out by Harvey [21]. In recent years, the existence of choking and shocks within the tip gap has been identified by Green et al [22], Molter et al…”
Section: B Problem Statement and Motivation Of The Present Workmentioning
confidence: 94%
“…There have been also other detailed experimental data and CFD analysis results with the moving casing showing a transonic nature of the over-tip flows, e.g. Green et al [22], Molter et al [23], and Tallman et al [24].…”
Section: High-load Blading Design With Relatively Low Tip Leakagementioning
“…Secondly the effectiveness of the tip treatments seems to lack a consistent and conclusive trend, given the relatively large amount of efforts already made on the relatively small suction side Mach number near or above the sonic condition has also been pointed out by Harvey [21]. In recent years, the existence of choking and shocks within the tip gap has been identified by Green et al [22], Molter et al…”
Section: B Problem Statement and Motivation Of The Present Workmentioning
confidence: 94%
“…There have been also other detailed experimental data and CFD analysis results with the moving casing showing a transonic nature of the over-tip flows, e.g. Green et al [22], Molter et al [23], and Tallman et al [24].…”
Section: High-load Blading Design With Relatively Low Tip Leakagementioning
“…Rotor exit conditions were obtained from (Ref. 18). Periodic boundaries were specified at the tangential boundaries.…”
Section: Steady Simulationmentioning
confidence: 99%
“…The exit pressure profile was obtained from a coarse grid 1½ stage unsteady simulation (Ref. 18). The exit total pressure and temperature profiles obtained from the steady simulation of the vane were circumferentially averaged.…”
In a previous study, vane-rotor shock interactions and heat transfer on the rotor blade of a highly loaded transonic turbine stage were simulated. The geometry consists of a high pressure turbine vane and a downstream rotor blade. This study focuses on the physics of flow and heat transfer in the rotor tip, casing, and hub regions. The simulation was performed using the unsteady Reynolds-averaged Navier–Stokes code MSU-TURBO. A low Reynolds number k-ε model was utilized to model turbulence. The rotor blade in question has a tip gap height of 2.1% of the blade height. The Reynolds number of the flow is approximately 3×106/m. Unsteadiness was observed at the tip surface that results in intermittent “hot spots.” It is demonstrated that unsteadiness in the tip gap is governed by inviscid effects due to high speed flow and is not strongly dependent on pressure ratio across the tip gap contrary to published observations that have primarily dealt with subsonic tip flows. The high relative Mach numbers in the tip gap lead to a choking of the leakage flow that translates to a relative attenuation of losses at higher loading. The efficacy of new tip geometry is discussed to minimize heat flux at the tip while maintaining choked conditions. In addition, an explanation is provided that shows the mechanism behind the rise in stagnation temperature on the casing to values above the absolute total temperature at the inlet. It is concluded that even in steady (in a computational sense) mode, work transfer to the near tip fluid occurs due to relative shearing by the casing. This is believed to be the first such explanation of the work transfer phenomenon in the open literature. The difference in pattern between steady and time-averaged heat fluxes at the hub is also explained.
“…Likewise, obtaining experimental measurements for heat transfer on the turbine shroud is extremely costly and difficult due to the high-temperature gradients as well as the size of the gap, as mentioned before. In the open literature, blade tip leakage flow has been studied over rotating blades [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15]. In addition, tip leakage flow has been investigated over stationary airfoils [16][17][18][19][20][21][22][23][24].…”
In today's modern gas turbine engines, the region between the rotor and the stationary shroud has the most extreme fluid-thermal conditions in the entire turbine and is characterized by a periodically unsteady threedimensional flowfield. The purpose of the present work is to conduct an unsteady study of the tip leakage flow adjacent to the shroud in real gas turbine engines using an in-house industrial computational fluid dynamics code. Both time-averaged and time-dependent data for the velocity, temperature, and mass flow rate in the tip clearance region are presented in parts 1 and 2, respectively. In part 1, it was found that near the pressure side of the tip clearance region and near the blade tip on the suction side, the leakage flow is dominant, whereas opposing flows entering through the suction side dominate near the shroud and at the suction side. This opposing flow is the combined effect of the shroud relative motion and the crossflow originating from the adjacent blade passage on the suction side. A small recirculation region was observed above the rotor passage and was attributed to the bladepassage crossflow interacting with the high-pressure region found at the suction side of the blade. This high-pressure region is caused by the combined effect of the crossflow with the shroud boundary-layer flow interacting with the tip leakage flow inside the tip clearance region. Nomenclature b = blade span C x = blade axial chord h = tip clearance height M = Mach number P = pressure r = radial coordinate T = temperature v = velocity vector W = mass flow rate x = axial coordinate y = Cartesian coordinate oriented along the circumferential direction z = Cartesian coordinate oriented along the radial direction Subscripts aw = adiabatic wall c = core flow o = stagnation properties rel = relative s = isentropic
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