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西安交通大学能源与动力工程学院, 710049,西安
Received:17 October 2024,
Online First:11 March 2025,
Published:10 July 2025
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LI Ke, ZHU Shun, WEN Jian. Effects of Vapor-Cooled Shields Integrated with Para-Ortho Hydrogen Catalytic Conversion on Self-Pressurization of Liquid Hydrogen Storage Tanks[J]. Journal of Xi’an Jiaotong University, 2025, 59(7): 170-181.
LI Ke, ZHU Shun, WEN Jian. Effects of Vapor-Cooled Shields Integrated with Para-Ortho Hydrogen Catalytic Conversion on Self-Pressurization of Liquid Hydrogen Storage Tanks[J]. Journal of Xi’an Jiaotong University, 2025, 59(7): 170-181. DOI: 10.7652/xjtuxb202507017.
为了有效提升液氢储罐的绝热性能,构建了真空多层绝热液氢储罐的瞬态传热传质模型,并研究了集成氢仲正催化转化的蒸气冷却屏的影响。引入蒸气消耗因子
η
c
、休眠期延长因子
η
d
等无量纲参数分别量化蒸气消耗量和储罐休眠期;定义单位因子
η
为
η
d
与
η
c
之比,表征蒸气冷却屏屏蔽漏热的能力。对比分析了有无仲正催化转化时蒸气冷却屏无量纲位置、质量流量和开启时刻等参数对储罐休眠期的影响。结果表明:
η
d
和
η
均随蒸气冷却屏无量纲位置的增大而先增大后减小;当
η
c
为0.012 8且蒸气冷却屏无量纲位置是0.167时,加入仲正催化转化相比未加入时的两个指标的增幅最大,为22.77%;随着蒸气冷却屏质量流量的减小,两个指标均先增大后减小;当蒸气冷却屏无量纲位置和蒸气冷却屏质量流量均较小时,加入仲正催化转化后两个指标的增幅较大;两个指标随着蒸气冷却屏开启时刻的推迟而先增大后减小;在
η
c
和蒸气冷却屏无量纲位置分别为0.025 6和0.233的条件下,蒸气冷却屏开启时刻设置为第40.51 d时,加入仲正催化转化后
η
的增幅最大为22.32%。
To effectively improve the thermal insulation performance of liquid hydrogen storage tanks
a transient heat and mass transfer model for vacuum multilayer insulated liquid hydrogen storage tanks is developed
and the effect of integrating a vapor-cooled shield with ortho-para hydrogen catalytic conversion is investigated. Dimensionless parameters
including the vapor consumption factor (
η
c
) and the dormancy period extension factor (
η
d
)
are introduced to quantify vapor consumption and tank dormancy period
respectively. A unit factor (
η
)
defined as the ratio of
η
d
to
η
c
is used to characterize the heat-leak shielding capability of the vapor-cooled shield. A comparative analysis is conducted on the effects of key parameters
such as the dimensionless position of the vapor-cooled shield
mass flow rate
and activation timing
on the tank dormancy period
with and without ortho-para catalytic conversion. The results indicate that: Both
η
d
and
η
initially increase and then decrease as the dimensionless position of the vapor-cooled shield increases; when
η
c
=0.012 8 and the dimensionless position of the vapor-cooled shield is
0.167
the inclusion of ortho-para catalytic conversion yields the maximum improvement in both metrics (22.77%) compared to the non-catalytic case; as the mass flow rate of the vapor-cooled shield decreases
both metrics first increase and then decrease; the improvement in both metrics is more pronounced when the dimensionless position and mass flow rate of the vapor-cooled shield are relatively small; both metrics initially increase and then decrease with delayed activation of the vapor-cooled shield; under conditions where
η
c
=0.025 6 and the dimensionless position of the vapor-cooled shield is 0.233
activating the shield at 40.51 d achieves the maximum improvement of 22.32% in
η
with ortho-para catalytic conversion.
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