赵昊城, 张泽秦, 王成龙, 秋穗正, 田文喜, 苏光辉. 基于有限体积法碱金属高温热管冷态启动流动换热数值研究[J]. 原子能科学技术, 2024, 58(1): 50-59. DOI: 10.7538/yzk.2022.youxian.0754
引用本文: 赵昊城, 张泽秦, 王成龙, 秋穗正, 田文喜, 苏光辉. 基于有限体积法碱金属高温热管冷态启动流动换热数值研究[J]. 原子能科学技术, 2024, 58(1): 50-59. DOI: 10.7538/yzk.2022.youxian.0754
ZHAO Haocheng, ZHANG Zeqin, WANG Chenglong, QIU Suizheng, TIAN Wenxi, SU Guanghui. Numerical Study on Flow and Heat Transfer of Alkali Metal High-temperature Heat Pipe during Frozen Startup Based on FVM[J]. Atomic Energy Science and Technology, 2024, 58(1): 50-59. DOI: 10.7538/yzk.2022.youxian.0754
Citation: ZHAO Haocheng, ZHANG Zeqin, WANG Chenglong, QIU Suizheng, TIAN Wenxi, SU Guanghui. Numerical Study on Flow and Heat Transfer of Alkali Metal High-temperature Heat Pipe during Frozen Startup Based on FVM[J]. Atomic Energy Science and Technology, 2024, 58(1): 50-59. DOI: 10.7538/yzk.2022.youxian.0754

基于有限体积法碱金属高温热管冷态启动流动换热数值研究

Numerical Study on Flow and Heat Transfer of Alkali Metal High-temperature Heat Pipe during Frozen Startup Based on FVM

  • 摘要: 为建立碱金属高温热管启动瞬态和运行稳态工作特性预测方法,本研究采用有限体积法(FVM)建立管壁导热模型、吸液芯流动传热模型和蒸气区模型。基于C语言开发并验证了碱金属高温热管的冷态启动瞬态分析程序,最大相对偏差为9.8%。仿真模拟了单根水平钠热管启动瞬态并开展敏感性分析,结果显示:对于本研究中使用的热管,在固定输入功率为1 000 W的环境条件下,启动开始后700 s热管蒸气区完全进入连续流态,到达稳态总用时为3 000 s,启动过程中工质熔化阶段吸液芯内部压力相对值逐渐增大,熔化完成后压力相对值略有降低;稳态运行下热管等温性良好,外壁面轴向温差稳定在22.5 K,吸液芯内部压降约为47 Pa;环境温度升高会延长热管到达稳态所需时间,并对稳态蒸气压力和流速分布产生一定影响;绝热段长度增加同样延长了热管启动到达稳态时间,同时对吸液芯内流体压力和速度分布存在一定影响。

     

    Abstract: In recent years, heat pipe has been widely used as an efficient heat transfer equipment in fuel chemistry, electronic communication and so on. The main structure of a heat pipe mainly includes the vacuum tube containing alkali metal working fluid and the composite mesh wick on the inner wall of the tube. In the axial direction, heat pipes are generally divided into three parts:evaporation section, adiabatic section and condensation section. Heat is input into the heat pipe through the evaporation section and output through the condensation section. The adiabatic section only plays a role in connecting and mass transfer. The length of each area can be flexibly arranged. In the radial direction, heat pipes are generally divided into outer wall surface, wick and vapor area. Alkali metal high-temperature heat pipes show broad application prospects in the nuclear reactor cooling and other aspects because of their strong heat transfer capacity and inherent safety at high temperature. Because the working fluid of these heat pipes is solid at room temperature, and whose saturated vapor pressure relatively low, their frozen start-up has a complex phase change process of the working fluid, so it brings some difficulties to the study of the frozen start-up of the high-temperature heat pipes. For different application scenarios, it is necessary to study the transient and steady-state operating characteristics of high-temperature heat pipes, to provide support for the application of high-temperature heat pipes in a variety of applicable scenarios. To establish a method for predicting the transient start-up and steady-state operation characteristics of alkali metal high-temperature heat pipes, this study utilized the finite volume method (FVM) to establish the pipe wall heat conduction model, the wick flow heat transfer model, and the vapor zone model. A frozen start-up transient analysis program for alkali metal high-temperature heat pipes was developed and verified using the C programming language, with a maximum relative deviation of 9.8%. Transient start-up of a single horizontal sodium heat pipe was simulated, and sensitivity analysis was conducted. The steam zone of the heat pipe enters the continuous flow state completely 700 seconds after start-up, and after a total of 3 000 seconds, the heat pipe reaches steady-state operation. Under steady-state operation, the heat pipe exhibits good isothermal properties, with a stable axial temperature difference of 22.5 K on the outer wall and an internal pressure drop of approximately 47 Pa in the wick. Furthermore, the ambient temperature primarily impacts the time required for the heat pipe to reach steady-state, as well as the vapor pressure and velocity distribution under steady-state conditions. Meanwhile, the length of the adiabatic section of the heat pipe influences the time required for it to reach steady-state and has a significant effect on the pressure and velocity distribution of the wick.

     

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