1. 华北电力大学动力工程系
2. 南方电网电力科技股份有限公司
3. 华北电力大学河北省低碳高效发电技术重点实验室
纸质出版:2026
移动端阅览
张硕, 李德波, 方立军, 等. 双接触式碳捕集气液两相吸收床氨法碳捕集传质过程模拟[J]. 热力发电, 2026,(5).
张硕, 李德波, 方立军, et al. 双接触式碳捕集气液两相吸收床氨法碳捕集传质过程模拟[J]. Thermal Power Generation, 2026, (5).
张硕, 李德波, 方立军, 等. 双接触式碳捕集气液两相吸收床氨法碳捕集传质过程模拟[J]. 热力发电, 2026,(5). DOI: 10.19666/j.rlfd.202508010.
张硕, 李德波, 方立军, et al. 双接触式碳捕集气液两相吸收床氨法碳捕集传质过程模拟[J]. Thermal Power Generation, 2026, (5). DOI: 10.19666/j.rlfd.202508010.
【目的】探究双接触式碳捕集气液两相吸收床强化氨法碳捕集传质性能。【方法】基于欧拉-拉格朗日CFD框架,结合双膜理论对Fluent进行二次开发,构建氨法碳捕集传质模型。【结果】液滴CO2负载沿塔高呈单峰分布,壁面低而中心高,且随液气比降低,CO2净通量增大,负载增大。烟气入口存在明显偏流,偏流程度随液气比减小而减弱,液滴分布不均导致CO2吸收与浓度场分布不均;液气比自0.40 m3/m3降至0.17 m3/m3时,CO2捕集率由89.19%降至77.29%,减小了13.34%,出口CO2摩尔分数由1.45%升至3.00%。气相总传质系数KG在床高3/4以下较高;喷嘴母管下方形成了带状低KG区;随液气比减小,整体上高KG区缩减,由喷嘴母管阻碍作用形成的带状低KG区呈上抛物线形态。流场方面,床内因入口与文丘里效应形成两处高速区及涡流,气相流速沿床高呈双峰分布,沿X方向为对称三段波动,沿Y方向呈非单调分布,液气比减小加剧了局部扰动及流速上升。【结论】双接触式碳捕集气液两相吸收床传质性能良好,液气比对流动与传质行为具有显著调控作用,研究结果可为碳捕集设备优化提供理论依据。
[Objective] At present
the greenhouse effect is becoming increasingly severe
making it crucial to control CO2 emissions from fossil fuel combustion. Carbon dioxide capture technology represents both the primary step and the critical pathway
serving as a vital means for reducing carbon emissions in the future. [Methods] Based on a novel double-contact carbon capture gas-liquid two-phase absorption bed
and to investigate its enhanced mass transfer performance for ammonia-based carbon capture
this study employs an Eulerian-Lagrangian CFD framework. By integrating dual-film theory into a secondary development of Fluent
a mass transfer model for ammonia-based carbon capture is constructed. [Results] The droplet load exhibits a unimodal distribution along the tower height
being low near the walls and high towards the center. As the liquid-to-gas ratio decreases
the net CO2 flux increases
leading to a higher droplet load. Significant flow deviation exists at the flue gas inlet
with its severity diminishing as the liquid-to-gas ratio decreases. The uneven droplet distribution causes non-uniformity in CO2 absorption and concentration field distribution. When the liquid-to-gas ratio decreases from 0.40 m3/m3 to 0.17 m3/m3
the CO2 capture efficiency drops from 89.19% to 77.29%
a reduction of 13.34%
while the outlet CO2 molar fraction rises from 1.45% to 3.00%. The overall gas-phase mass transfer coefficient(KG) remains relatively high below three-quarters of the bed height. A banded region of low KG forms beneath the nozzle manifold. In the region above the nozzles
KG gradually decreases with increasing bed height due to insufficient mass transfer driving force and the influence of mass transfer resistance from the gas film side. As the liquid-to-gas ratio decreases
the high KG zone contracts
and the banded low KG zone exhibits a parabolic upward trajectory. Regarding the flow field
two high-velocity zones and vortices form within the bed due to the inlet and Venturi effect. The average gas phase velocity in the Z-direction exhibits a bimodal distribution along the bed height
a symmetrical three-segment oscillation along the X-cross section
and a non-monotonic distribution along the Y-cross section. As the liquid-togas ratio decreases
the disturbance between the gas and liquid phases intensifies
causing the average gas phase velocity along the Y=0 cross section and the X-cross section to gradually increase. [Conclusion] The double-contact carbon capture gas-liquid two-phase absorption bed exhibits favourable mass transfer characteristics
with the liquid-to-gas ratio exerting a significant regulatory effect on both flow and mass transfer. These findings provide a theoretical basis for optimizing carbon capture equipment.
0
浏览量
280
下载量
0
CSCD
关联资源
相关文章
相关作者
相关机构
京公网安备11010802024621