水泵水轮机转轮内空化流动诱导压力脉动及径向力特性研究

Study on Cavitation Flow-Induced Pressure Pulsation and Radial Force Characteristics Within the Pump-Turbine Runner

  • 摘要: 为研究水泵水轮机转轮内空化流动对压力脉动和叶片受力的影响,采用MSST PANS模型在 NPSHa=1.71~10.01范围内对泵工况进行非定常数值模拟. 经过网格和时间步长无关性验证,模拟扬程相比实验误差小于 2.3%. 当NPSHa>NPSHc(临界空化余量)时,压力脉动峰峰值从流道进口到出口逐渐增大,表明动静干涉是诱发压力脉动的主要原因. 当NPSHa<NPSHc时,转轮内空化流动导致压力脉动骤增,其峰峰值从NPSHc时的4.9%增至NPSHa=1.71时的11.2%,且最大压力脉动峰峰值所在的位置动态变化;此时,空化引起转轮内体积流量波动,导致流动紊乱并伴随大量涡结构生成. 对于径向力,其在NPSHa≥NPSHc范围内几乎不随进口压力改变而发生变化,相对波动小于2%;但NPSHa<NPSHc时,径向力主频为空化流动诱导的低频,径向力相较于无空化时的增幅约为6.9%~21.1%.

     

    Abstract: To investigate the impact of cavitation flow within a pump-turbine runner on pressure pulsations and blade loading, unsteady numerical simulations were conducted under pump operating conditions using the MSST PANS model, covering a net positive suction head available (NPSHa) range of 1.71 to 10.01. After grid and time-step independence verification, the discrepancy between the simulated head and experimental results was less than 2.3%. When NPSHa exceeded the critical cavitation margin (NPSHc), the peak-to-peak pressure pulsation amplitude gradually increased from the flow channel inlet to the outlet, indicating that rotor-stator interaction is the primary cause of pressure pulsations. When NPSHa fell below NPSHc, cavitation flow within the runner led to a sharp increase in pressure pulsations, with the peak-to-peak value rising from 4.9% at NPSHc to 11.2% at NPSHa=1.71. Furthermore, the location of the maximum peak-to-peak pressure pulsation shifted dynamically. Under these conditions, cavitation induced fluctuations in the volumetric flow rate within the runner, resulting in flow disorder and the generation of numerous vortex structures. Regarding radial forces, within the range of NPSHa ≥ NPSHc, they remained largely unaffected by changes in inlet pressure, with relative fluctuations below 2%. However, when NPSHa < NPSHc, the dominant frequency of the radial forces shifted to a low frequency induced by cavitation flow, and the magnitude of the radial forces increased by approximately 6.9% to 21.1% compared to non-cavitation conditions.

     

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