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Thermodynamic and economic analysis of a novel hydrogen liquefaction process with LNG precooling and dual-pressure Brayton cycle

布莱顿循环 液化 火用 液化天然气 气体压缩机 可用能 环境科学 废物管理 能源消耗 核工程 透平膨胀机 工艺工程 液态氢 工程类 化学 天然气 机械工程 热交换器 有机化学 电气工程 岩土工程
作者
Jiang Bian,Jian Yang,Yuxing Li,Zhaoqi Chen,Fachun Liang,Xuewen Cao
出处
期刊:Energy Conversion and Management [Elsevier BV]
卷期号:250: 114904-114904 被引量:90
标识
DOI:10.1016/j.enconman.2021.114904
摘要

• The direct expansion cycle of liquified natural gas was used to pre-cool hydrogen. • A novel dual-pressure Brayton cascade cycle was designed for hydrogen cryo-cooling. • The investment costs of different processes were compared by economic indicators. • The proposed process showed advantages in energy consumption, costs, and efficiency. • The exergy analysis and parameter studies of the proposed process were carried out. Liquid hydrogen with high energy density and cleanliness is a superior alternative to current energy carriers. However, high costs and low efficiency are barriers to liquefy hydrogen. To reduce the energy consumption and investment costs of hydrogen liquefaction, a hydrogen liquefaction process that utilizes a direct expansion cycle of liquefied natural gas for hydrogen precooling and a dual-pressure Brayton cascaded cycle for hydrogen cryo-cooling is proposed. The hydrogen liquefaction performance and economic benefits of the proposed process are assessed by comparing it with two reference processes with different cryo-cooling cycles. The results reveal the advantageous operating costs and capital costs of the proposed process, especially in terms of the costs of helium and heat exchangers. Moreover, the specific energy consumption of the proposed process is 6.60 kWh/kg H2 , which is 4.0% and 4.5% lower than those of the reference processes. The exergy losses and exergy efficiency of the proposed process are 12.36 MW and 47.0%, respectively, and the exergy losses are mainly caused by the compressors and expanders. The energy consumption of the proposed process decreases at first and subsequently increases with the increasing pre-compression pressure of helium.
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