液态金属相变逆流换热器中的热和粘性不可逆分析

Élcio Nogueira, Diniz Felix dos Santos Filho
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引用次数: 0

摘要

钠是一种液态金属,在与核反应堆相连的热交换器系统中用于生产氢气。过冷液态金属进入逆流热交换器,发生相变,然后以过热蒸汽的形式排出。钠的加热过程是通过与过热氦蒸气进行热交换实现的,热交换分为三个阶段:过冷液体、饱和蒸气和过热蒸气。本文采用分析模拟法,通过热不可逆和粘性不可逆来分析热交换器三个阶段的热性能和水力性能。根据热效率法和热力学第二定律得出了解决方案。热力学贝扬数是热不可逆性和总不可逆性之间的关系,可以在确定热性能和粘性耗散时进行成本效益分析。分析中使用的基本物理量是热交换器三个部分的长度和内径。分析结果与之前发表在文献中的分析工作进行了比较。获得了温度曲线、热效率、传热速率、热不可逆性、压降、粘性不可逆性、熵生成率和贝扬数的数值和图形结果。结果表明,当三段内部管道的直径等于饱和钠蒸气段的直径(相当于管内声速的 ¼)时,成本效益非常高。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Thermal and Viscous Irreversibilities Analysis in a Liquid Metal Phase Change Counter Flow Heat Exchanger
Sodium, a liquid metal, is utilized in a heat exchanger system coupled to a nuclear reactor to produce hydrogen. The subcooled liquid metal enters a counterflow heat exchanger, undergoes a phase change, and exits as superheated vapor. The sodium heating process occurs through heat exchange with superheated helium vapor in three phases: subcooled liquid, saturated vapor, and superheated vapor. This article analyzes the thermal and hydraulic performance of the three stages of the heat exchanger through thermal and viscous irreversibilities using analytical simulation. The solution obtained is based on applying the thermal efficiency method and the second law of thermodynamics. The thermodynamic Bejan number, the relationship between thermal irreversibility and total irreversibility, allows a cost-benefit analysis when determining thermal performance and viscous dissipation. The essential physical quantities used in the analysis are the lengths and internal diameters of the three segments of the heat exchanger. The results are analyzed and compared with previous analytical work published in the literature. Numerical and graphical results are obtained for temperature profiles, thermal effectiveness, heat transfer rate, thermal irreversibilities, pressure drops, viscous irreversibilities, entropy generation rate, and Bejan numbers. It is demonstrated that the cost-benefit is highly advantageous when the diameter used for the internal tubes of the three segments is equal to the diameter of the saturated sodium vapor section, corresponding to ¼ of the speed of sound in the tube.
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