1.石家庄铁道大学机械工程学院,河北省低温储能重点实验室
2.石家庄铁道大学, 河北省新型储能国际联合研究中心
3.石家庄铁道大学材料科学与工程学院, 河北 石家庄 050043
刘斌(1985—),男,博士,副教授,研究方向为氨氢燃烧技术,E-mail:liubin@stdu.edu.cn;
周娜,博士,副教授,研究方向为氨氢融合催化剂,E-mail:chmzhouna@stdu.edu.cn。
收稿:2026-04-18,
修回:2026-05-28,
纸质出版:2026-09-28
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刘斌, 张思超, 周娜, 等. 氨-氢燃烧驱动氨分解能量利用率的多指标评估[J]. 储能科学与技术, 2026, 15(9): 3750-3761.
LIU Bin, ZHANG Sichao, ZHOU Na, et al. Multi-index evaluation of energy utilization rate in ammonia-hydrogen combustion-driven ammonia decomposition[J]. Energy Storage Science and Technology, 2026, 15(9): 3750-3761.
刘斌, 张思超, 周娜, 等. 氨-氢燃烧驱动氨分解能量利用率的多指标评估[J]. 储能科学与技术, 2026, 15(9): 3750-3761. DOI: 10.19799/j.cnki.2095-4239.2026.0337.
LIU Bin, ZHANG Sichao, ZHOU Na, et al. Multi-index evaluation of energy utilization rate in ammonia-hydrogen combustion-driven ammonia decomposition[J]. Energy Storage Science and Technology, 2026, 15(9): 3750-3761. DOI: 10.19799/j.cnki.2095-4239.2026.0337.
针对氨-氢燃烧放热与氨催化分解吸热过程之间的能量匹配和利用效率问题,建立了氨-氢燃烧驱动氨分解的燃烧-分解耦合计算流体力学模型,并构建了能量利用率评价方法。模型中燃烧区采用氨-氢-空气Duynslaegher气相反应机理,分解区视为填充Ni-Pt/Al
2
O
3
催化剂的多孔介质反应区,同时考虑燃烧放热、氨分解吸热、组分输运、辐射传热及两区间热量传递过程。通过与文献实验数据对比,验证了所建模型对氨分解耦合过程的预测可靠性。在此基础上,系统考察了分解区入口速度、燃烧区入口速度以及燃烧区与分解区尺寸比例对温度场分布、氨分解率、燃烧区出口温度和能量分配与效率的影响。结果表明,引入氨分解后,分解反应的吸热作用能够重构燃烧区温度场,使燃烧区峰值温度降低100~150 K,分解区径向温差维持在4.3~4.4 K,有利于削弱局部高温集中并降低反应器材料热负荷。当燃烧区入口速度保持不变,分解区入口速度由0.1 m/s 增加至1.0 m/s 时,氨分解率由99.98%降至66.24%,燃烧区出口温度由1053 K降至984 K,但由于尾气带走的热量减少,更多燃烧热被转化为氨分解吸热,系统能量利用率呈先升高后降低的趋势,最大提升约22%。当分解区入口速度固定,燃烧区入口速度由0.1 m/s提高至0.5 m/s时,氨分解率由66.24%提高至99.99%,燃烧区出口温度由984 K上升至1614 K,过量热输入主要随尾气排出,导致有效能量利用率下降。尺寸比例分析表明,燃烧区与分解区尺寸比例由1∶2增大至2∶1时,分解区停留时间由4.00 s缩短至1.00 s,气时空速由900 h
-
¹增至3600 h
-
¹,氨分解率由96%降至66%,说明停留时间缩短是分解性能下降的主导因素。本研究建立的多指标评价方法能够揭示燃烧供热、氨分解吸热与氢气化学能产出之间的能量转化关系,可为氨-氢耦合反应器的结构优化提供参考。
A coupled combustion-decomposition computational fluid dynamics model is established to address energy-matching and utilization-efficiency challenges between exothermic ammonia-hydrogen combustion and endothermic ammonia catalytic decomposition. Additionally
a method for evaluating energy-utilization efficiency is developed. In the model
the combustion zone adopts the ammonia/hydrogen/air Duynslaegher gas-phase reaction mechanism
while the decomposition zone is modeled as a porous-medium reaction zone packed with an Ni-Pt/Al
2
O
3
catalyst. The model accounts for combustion heat release
ammonia-decomposition heat absorption
component transport
radiative heat transfer
and heat transfer between the two zones. The prediction reliability of the model for the coupled ammonia-decomposition process is validated against experimental data from the literature. On this basis
the effects of the decomposition-and combustion-zone inlet velocities
as well as the ratio of the size of the combustion zone to that of the decomposition zone
on the temperature-field distribution
ammonia-decomposition rate
combustion-outlet temperature
and energy-distribution efficiency are systematically investigated. Results show that integrating ammonia decomposition reconstructs the combustion temperature field
suppressing the peak temperature by 100—150 K while maintaining a radial decomposition-temperature difference at 4.3—4.4 K. This thermal leveling mitigates localized high-temperature concentrations and reduces the thermal load on the reactor material. When the combustion inlet velocity is kept constant while the decomposition inlet velocity increases from 0.25 to 1.0 m/s
the ammonia-decomposition rate decreases from 99.98% to 66.24%
and the combustion outlet temperature decreases from 1053 to 984 K. However
the decreased heat released by the exhaust gas and the conversion of more combustion heat into ammonia-decomposition heat absorption allow the system's energy-utilization efficiency to follow a trend of first increasing and then decreasing
peaking at approximately 22% gain. When the decomposition inlet velocity is fixed and the combustion inlet velocity increases from 0.1 to 0.5 m/s
the ammonia-decomposition rate increases from 66.24% to 99.99% but surges the combustion outlet temperature to 1614 K. The excess heat input is mainly discharged with the exhaust gas
causing a decrease in the effective energy-utilization proportion. The size-ratio analysis indicates that increasing the combustion-to-decomposition size ratio from 1∶2 to 2∶1 shortens the decomposition-zone residence time from 4.00 to 1.00 s while increasing the gas hourly space velocity from 900 to 3600 h
-1
. Consequently
the ammonia-decomposition rate decreases from 96% to 66%
establishing residence-time reduction as the dominant factor governing the decline in decomposition performance. The established multi-index evaluation framework elucidates the energy-conversion dynamics between combustion heat supply
ammonia-decomposition heat absorption
and hydrogen chemical en
ergy output
providing a reference for the structural optimization of coupled ammonia-hydrogen reactors.
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