An accurate prediction of the performance characteristics of cavitating cryogenic turbopump inducers is essential for an increased reliance on numerical simulations in the early turbopump design stages of liquid rocket engines. This work focuses on the sensitivities related to the choice of turbulence models on the cavitation prediction in flow setups relevant to cryogenic turbopump inducers. To isolate the influence of the turbulence closure models for Reynolds-averaged Navier-Stokes equations, four canonical problems are abstracted and studied individually to separately consider cavitation occurring in flows with a bluff body pressure drop, adverse pressure gradient, blade passage contraction and rotation. The choice of turbulence model plays a significant role in the prediction of the phase-distribution in the flow. It was found that the sensitivity to the closure model depends on the choice of cavitation model itself; the barotropic-based cavitation models are far more sensitive to the turbulence closure than the transportbased models. The sensitivity of the turbulence model is also strongly dependent on the type of flow. For bounded cavitation flows (blade passage), stark variations in the cavitation topology are observed based on the selection of the turbulence model. For unbounded problems, the spread in the results due to the choice of turbulence models is similar to non-cavitating, single-phase flow cases. A set of considerations for turbopump designers are provided for an informed decision on the selection of turbulence models. * Corresponding author
IntroductionTurbopumps in liquid rocket engines (LRE) deliver propellants, such as liquid hydrogen (LH2) and liquid oxygen (LO2), from low pressure storage tanks to a high pressure combustion chamber [1]. They are a central component in LREs as they control both injection pressure and propellant mass flow rate to the combustor. The design and analysis of turbopumps is highly complex due to high rotational speeds, and potential for the onset of vibrations and flow instabilities while simultaneously needing to meet the stringent performance and weight requirements of the system [1,2].The mass and size constraints imposed to the turbopump means that a high rotational speed (often over 20,000 rpm) is needed in order to deliver the required mass flow rate of propellants to the combustor. Because of the high rotational speeds, cavitation is likely to arise on the suction side of the blade passages as the static pressure of the liquid drops down to its vapour pressure [1]. Cavitation is to be avoided as it leads to a reduction of the pump efficiency, mixing losses, erratic mass flow rate, insufficient power to the fluid, and can result in dangerous vibrations and instabilities. In a turbopump assembly, an axial impeller called inducer is placed in front of the main impeller on the same shaft with the same rotational speed [1]. The inducer marginally increases the liquid pressure such that cavitation is avoided or severely reduced at the main impeller inl...