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基于开放边界条件的离心泵自吸过程瞬态流动数值模拟

Numerical investigation on transient characteristics of self-priming process in a centrifugal pump using opening boundary conditions

  • 摘要: 为探明泵内气液两相瞬态流动特征及自吸过程中吸水管液面震荡上升机理,该研究基于欧拉-欧拉多相流均相模型及标准k-ε湍流模型,采用开放型进、出口边界,对某外混式自吸离心泵在变转速启动条件下的自吸过程进行了数值模拟,分析了吸水管液面变化和主要过流部件内气液两相分布等瞬态特征。结果表明,开放型边界条件可以准确捕捉自吸过程中吸水管内液面震荡上升现象,与试验结果吻合良好。自吸过程包含3个阶段:快速吸入阶段对应吸水室内初始储液被快速吸入叶轮并将叶轮内气体排出,占自吸总用时的11.7%;震荡排气阶段是泵自吸过程的主要阶段,占总自吸时间的61.3%,该阶段内气液分离室内液体反复进入蜗壳和叶轮外缘区域,参与气液掺混及气液分离过程,完成自吸排气,过流部件内气液两相占比及吸水管液面震荡均近似呈0.25 s的周期性变化,叶轮内气相占比周期性变化和液柱惯性是导致该自吸阶段吸水管内液面震荡的主要原因;加速排气阶段为自吸末期,吸水管内液体加速进入叶轮,将泵内气体快速排出,其历时占总自吸时间的27%。研究结果可为自吸泵设计及性能优化提供重要参考。

     

    Abstract: This study aims to explore the gas-liquid two-phase flows during the self-priming process in an external-mixing self-priming centrifugal pump using Euler-Euler modeling, with an emphasis on the transient flow characteristics and the underlying mechanisms for the oscillating of the gas-liquid interface in the suction pipe. A homogeneous multiphase model (without considering the interphase velocity slip), and the standard k-ε turbulence model were adopted in the simulation. The opening boundary conditions were applied for the fluid at the inlet and outlet of the calculation domain, in order to capture the rising process of liquid level in the suction pipe. The speed was measured to determine the rotating speed of the rotor. The speed acceleration was then performed on the self-priming during the start-up process of the pump. The transient flow fields of the main components were investigated to reveal the gross features of the gas-liquid interface rising in the suction pipe, the mass flow rate of the liquid at the impeller inlet, the average gas volume fractions of pump components, and gas-liquid distribution in the flow passage of the pump. The simulated rising process of the gas-liquid interface in the suction pipe was agreed well with the experimental measurements. It infers that the opening boundary conditions were suitable for the reverse flow in the suction pipe caused by pressure oscillation in the impeller. The transient liquid phase flow rate at the impeller inlet indicated that the self-priming process was divided into three stages, namely the rapid absorbing, the oscillating exhaust, and the accelerating exhaust stage. The duration of the three stages accounted for 11.7%, 61.3% and 27% of the total self-priming time, respectively. The impeller rotating speed increased sharply at the rapid absorbing stage, where the initially stored liquid in the suction chamber was quickly sucked into the impeller to discharge the gas in the impeller. The oscillating exhaust was the main stage of the self-priming process, where the liquid in the gas-liquid separation chamber repeatedly entered the volute and the vicinity of the impeller outlet through the reflux hole in the process of gas-liquid mixing and gas exhausting. There was a periodic change with 0.25 s in the volume fraction of gas in the main pump components and the oscillation of liquid level in the suction pipe. But the inertia of the liquid column caused a phasegap between the liquid level oscillation and the pressure fluctuation at the impeller entrance. The oscillation amplitude of the gas-liquid interface increased with the increase of liquid column height. The accelerating exhaust stage was the final stage of the self-priming process, where the liquid in the suction pipe rapidly entered the impeller and the gas in the pump was quickly discharged. The finding can also provide an important reference for the design and performance optimization of self-priming centrifugal pumps.

     

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