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The paper focuses on the unsteady pressure field measured around the rotor midspan profile of the VKI Brite transonic turbine stage. The understanding of the complex unsteady flow field is supported by a quasi-three-dimensional unsteady Navier–Stokes computation using a k-ω turbulence model and a modified version of the Abu-Ghannam and Shaw correlation for the onset of transition. The agreement between computational and experimental results is satisfactory. They both reveal the dominance of the vane shock in the interaction. For this reason, it is difficult to identify the influence of vane-wake ingestion in the rotor passage from the experimental data. However, the computations allow us to draw some useful conclusions in this respect. The effect of the variation of the rotational speed, the stator–rotor spacing, and the stator trailing edge coolant flow ejection is investigated and the unsteady blade force pattern is analyzed.

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The aerothermal performance of highly loaded high-pressure turbines is abated by the unsteady impact of the vane shocks on the rotor. This paper presents a detailed physical analysis of the stator-rotor interaction in a state-ofthe-art transonic turbine stage at three pressure ratios. The experimental characterization of the steady and unsteady flowfield was performed in a compression tube test rig. The calculations were performed using ONERA's code elsA. This original comparison leads to an improved understanding of the complex unsteady flow physics of a high-pressure turbine stage. The vane shock impingement on the rotor originates a separation bubble on the rotor crown that is responsible for the generation of high losses. A model based on rothalpy conservation has been used to assess the pressure loss. The analysis of the unsteady forcing relates the shock patterns with the force fluctuations. NomenclatureH = turbine span height, m M is = isentropic Mach number Nu = Nusselt number P = pressure, Pa S = curvilinear abscissa along wall surface, m T = temperature, K T r = rotor passing period, s T rotation = wheel rotation period, s T s = stator passing period, s t = time, s x = turbine axial direction, m y = turbine radial direction, m y = normalized distance of first wall cell Subscripts w = wall s = static 0 = freestream, total conditions 1 = stator inlet 2 = stator-rotor interface 3 = rotor outlet

In high-pressure turbines, a small amount of cold flow is ejected at the hub from the cavity that exists between the stator and the rotor disk. This prevents the ingestion of hot gases into the wheel-space cavity, thus avoiding possible damage. This paper analyzes the interaction between the hub-endwall cavity flow and the mainstream in a high-pressure transonic turbine stage. Several cooling flow ratios are investigated under engine representative conditions. Both time-averaged and time-resolved data are presented. The experimental data is successfully compared with the results of a three-dimensional steady Navier-Stokes computation. Despite the small amount of gas ejected, the hub-endwall cavity flow has a significant influence on the mainstream flow. The Navier-Stokes predictions show how the ejected cold flow is entrained by the rotor hub vortex. The time-resolved static pressure field around the rotor is greatly affected when traversing the non-uniform vane exit flow field. When the cavity flow rate is increased, the unsteady forces on the rotor airfoil are reduced. This is linked to the decrease of vane exit Mach number caused by the blockage of the ejected flow.