Cascade Flow Research Capability Following figures present experimental results dealing with the measurement of boundary layer development along the suction surface of a low pressure turbine blade under periodic unsteady wake flow conditions. For more details, please see the publication list in CV CV of Dr. Schobeiri TPFL: Turbine Cascade Unsteady Boundary Layer Research

Introduction: Wake Interaction  Boundary transition in turbomachines is determined by:  Change of frame of reference that inherently causes periodic unsteady flow consisting of wakes with high TI- vortical cores and low TI- flow region  Wake flow impinges on the surface of the following cascade and periodically changes the portion of the laminar boundary layer to turbulent and affects the turbine aerodynamics, efficiency, performance and heat transfer Schematics of Rotor-Stator Interaction

TPFL: The Turbomachinery Performance and Flow Research Laboratory Texas A&M University M. T. Schobeiri TPFL Unsteady Turbine Cascade Research Facility Simulation of periodic unsteady wakes impinging on turbine blades

INTRODUCTION: LOW-PRESSUER TURBINE AERODYNAMICS Fig. 1: A twin-spool aircraft gas turbine with a fan-stage, HP, IP, and LP compressor and turbine stages Low Pressure Turbine (LPT) stage of aircraft gas turbine engines operates within the following Re-range:  Take off: Re = 400,000 (high Re)  Cruise: Re = 100,000(low Re)  Routine operationsRe = 400,000 to 100,000 LP-Turbine

Introduction: LPT-Aerodynamics On Suction surface: Negative pressure gradient: Acceleration, stable laminar boundary layer Change of pressure gradient: Onset of a separation bubble, manifestation Further change of pressure gradient: Re-attachment of separated flow Fig. 3: Pressure distribution Fig. 2: LPT-blade, suction side Suction Surface Pressure Surface

Parameters Affecting LPT-Aerodynamics Flow parameters:  Re Number, Mach Number  Unsteady Wakes - Wake Frequency - Wake Width - Wake Turbulence  Freestream Turbulence Intensity Blade geometry:  Suction, pressure surface configuration (front, aft-load)  Inlet, exit angle (total flow deflection) - Responsible for pressure distribution, location of separation bubble

RESEARCH OBJECTIVES  To investigate the impact of the periodic unsteady inlet flow conditions on the development of the boundary layer separation.  To provide detailed steady and unsteady boundary flow information to understand the underlying physics of the onset and the extent of the separation zone under the unsteady wake effects.  To extend the intermittency based unsteady boundary layer transition model developed by Schobeiri and his co-workers to the boundary layer cases with separation.  To create a bench mark data base for comparison with numerical computation using DNS or RANS-codes.

UNSTEADY FLOW TURBINE CASCADE RESEARCH FACILITY

SIMULATION OF PERIODIC UNSTEADY WAKE FLOW CONDITION

RESULTS AND DISCUSSIONS:Unsteady Wake Flow Investigations Time-averaged velocity profiles along the suction surface of the blade at Ω=0

Periodic Generation and Suppression of the Separation Bubble Contour plot of the ensemble averaged velocity distribution showing the effect of periodic wakes an the separation zone at different streamwise positions at Ω =1.59

Periodic Generation and Suppression of the Separation Bubble Contour plot of the ensemble averaged velocity distribution showing the effect of periodic wakes an the separation zone at different streamwise positions at Ω =1.59

Temporal behavior of the separation zone behavior unsteady case Ω =1.59 (S R =160mm) Periodic Generation and Suppression of the Separation Bubble

Temporal behavior of the separation zone behavior unsteady case Ω =1.59 (S R =160mm). Note the development of the separation bubble. Periodic Generation and Suppression of the Separation Bubble

Physics of Contraction, Separation and Regeneration of the Separation Zone Periodic Generation and Suppression of the Separation Bubble

Contraction, Separation and Regeneration of the Separation Zone More Details on Generation and Suppression of the Separation Bubble

Periodic Generation and Suppression of the Separation Bubble Details: Contraction phase starts at the point, where  v rms /  t > 0 start, Regeneration phase starts at the point, where of  v rms /  t < 0 starts

Boundary layer ensemble-averaged integral momentum deficiency thickness for steady case Ω =0 (S R =  )and unsteady cases Ω =1.59(S R =160mm) and Ω =3.18 (S R =80mm) Boundary Layer Integral Quantities

Boundary layer momentum thickness time-averaged Boundary Layer Integral Quantities