Abstract

The stuck shaft accident (SSA) is a typical and severe accident of the reactor coolant pump (RCP). During this accident, significant friction and heat generation result in gas–liquid two-phase flow, which adversely affects the working performance and stability of the RCP. In order to explore the internal flow field and transient pressure fluctuation of the two-phase flow in the RCP under the SSA, this study adopts three methods of standard k-ε, Large Eddy Simulation (LES) and Lattice Boltzmann Method-Large Eddy Simulation (LBM-LES) for refined simulation and then are validated by experiments. It finds that the gas volume fraction (GVF) is relatively high in the inlet path of the guide vane during the initial stage, and then the gas disperses from the suction surface of the impeller blade to the pressure surface. When the GVF increases, the small gas masses accumulate into large masses and collapses in the RCP. At this time, the vorticity in the impeller path increases and then decreases at the outlet. The pressure fluctuation on the pressure surface at the impeller outlet increases with the increase of GVF. The impact of the GVF on the pressure surface is greater than that on the suction surface, particularly in the high-frequency band during the initial stages of the SSA. Among these three models, LBM-LES demonstrates the highest accuracy with a maximum deviation of only 8.84% when the inlet GVF is 10%. The research results improve the prevention and mitigation ability of related accidents, and provide theoretical basis and technical support for subsequent optimization and improvement.

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