郭梁,陈烨,贾启明,等. 液氢贮罐内过热蒸气不同质量流量泄放过程模拟[J]. 真空与低温,2024,30(4):392−397. DOI: 10.12446/j.issn.1006-7086.2024.04.007
引用本文: 郭梁,陈烨,贾启明,等. 液氢贮罐内过热蒸气不同质量流量泄放过程模拟[J]. 真空与低温,2024,30(4):392−397. DOI: 10.12446/j.issn.1006-7086.2024.04.007
GUO L,CHEN Y,JIA Q M,et al. Simulation of the venting process with different mass flow rates of superheated vapor in a liquid hydrogen storage tank[J]. Vacuum and Cryogenics,2024,30(4):392−397. DOI: 10.12446/j.issn.1006-7086.2024.04.007
Citation: GUO L,CHEN Y,JIA Q M,et al. Simulation of the venting process with different mass flow rates of superheated vapor in a liquid hydrogen storage tank[J]. Vacuum and Cryogenics,2024,30(4):392−397. DOI: 10.12446/j.issn.1006-7086.2024.04.007

液氢贮罐内过热蒸气不同质量流量泄放过程模拟

Simulation of the Venting Process with Different Mass Flow Rates of Superheated Vapor in a Liquid Hydrogen Storage Tank

  • 摘要: 以液氢工厂中贮存液氢的液氢贮罐为研究对象,选择液氢、气液相界面、蒸气三个区域合适的控制方程,建立了可模拟从自增压到泄放后回到初始压力过程的三区模型。模拟了充液率为50%的10 m3液氢贮罐从自增压-泄放后回到初始压力的周期过程。在特定泄放时间,不同泄放质量流量条件下,对比了液氢贮罐内贮罐压力、饱和液氢和过热蒸气的质量流量和温度以及液氢体积随时间的变化特性。结果表明:泄放过热蒸气质量流量大小随泄放时间增大不断减小;泄压时间越短,泄放后过热蒸气温度越接近初始温度;进入泄放阶段,蒸发液氢质量流量发生了明显激增,增大幅度随泄放时间增大而减小。

     

    Abstract: The liquid hydrogen storage tank in a liquid hydrogen plant is taken as the object of study, and a three-zone model is established for calculations by choosing suitable control equations for three zones: liquid hydrogen, gas-liquid phase interface and superheated flash vapor. The simulation of a 10 m3 liquid hydrogen storage tank with a 50% filling rate is carried out from the self-pressurization process to the first venting to the initial pressure. The characteristics of the tank pressure, the mass flow rates of saturated liquid hydrogen and superheated flash vapor, the temperature, and the volume of the liquid hydrogen storage tank are compared with each other for different venting mass flow rates at a specific venting time. The results show that the mass flow rate of superheated flash vapor decreases with the increase of the venting time, the shorter the pressure venting time is, the closer the superheated flash vapor temperature is to the initial temperature after the venting, the mass flow rate of the boiled liquid hydrogen undergoes a significant surge during the venting stage, and the magnitude of the increase decreases with the increase of the venting time.

     

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