1. 云南电网有限责任公司电力科学研究院,昆明,650217
2. 武汉大学电气与自动化学院,武汉,430072
收稿:2026-07-31,
纸质出版:2026
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邱方程, 王琳, 郑欣, 等. 优化气路结构下三维滑动弧等离子体的固氮效率[J]. 高电压技术, 2026,52(7):3458-3467.
QIU Fangcheng, WANG Lin, ZHENG Xin, et al. 优化气路结构下三维滑动弧等离子体的固氮效率[J]. 2026, 52(7): 3458-3467.
邱方程, 王琳, 郑欣, 等. 优化气路结构下三维滑动弧等离子体的固氮效率[J]. 高电压技术, 2026,52(7):3458-3467. DOI: 10.13336/j.1003-6520.hve.20251420.
QIU Fangcheng, WANG Lin, ZHENG Xin, et al. 优化气路结构下三维滑动弧等离子体的固氮效率[J]. 2026, 52(7): 3458-3467. DOI: 10.13336/j.1003-6520.hve.20251420.
氮是生命体必需元素,但自然界中的氮主要以稳定的氮气(N2)形式存在,难以被直接利用,因此须将其转化为含氮化合物,即固氮过程。目前工业固氮普遍存在高能耗和高污染等问题。为此,设计了一种气驱滑动弧放电等离子体装置,用于高效固氮实验研究。该装置的放电模式包括稳定滑动(steady arc gliding,A-G)模式和击穿伴随滑动(breakdown gliding,B-G)模式。通过示波器采集不同工作参数下的电压与电流信号,并利用相机记录2种模式的放电形态。系统研究了电源输出功率、进气流量及原料气体中氧气含量对固氮效率的影响,并对不同放电模式进行了对比分析。结果表明,B-G模式具有较低的能耗特征,但氮氧化物产率偏低;而A-G模式可显著提高氮氧化物浓度,但对应能耗较高。因此,在实际应用中应根据具体需求选择合适的工作模式。通过优化放电参数,产物中氮氧化物体积分数由4 180×10−6提升至12 097×10−6,增加约189%;固氮能耗由4.6 MJ/mol降至2.4 MJ/mol,降低约50%,显著提升了等离子体固氮效率。
Nitrogen is an essential element for living organisms
but in nature
it mainly exists in the stable form of nitrogen gas (N2)
which is difficult to be directly utilized. Therefore
it needs to be converted into nitrogen-containing compounds
a process known as nitrogen fixation. At present
industrial nitrogen fixation generally suffers from high energy consumption and serious pollution problems. To address this issue
a gas-driven gliding arc plasma device was designed in this study for efficient nitrogen fixation research. The discharge modes of the device include the steady arc gliding (A-G) mode and the breakdown gliding (B-G) mode. The voltage and current signals under different operating parameters were collected using an oscilloscope
and the discharge patterns of the two modes were recorded using a camera. The effects of power output
gas flow rate
and oxygen content in the feed gas on nitrogen fixation efficiency were systematically investigated
and the differences between the two discharge modes were compared. The results show that the B-G mode features lower energy consumption but a relatively low yield of nitrogen oxides
while the A-G mode can significantly increase the nitrogen oxide concentration but at a higher energy cost. Therefore
in practical applications
an appropriate discharge mode should be selected on the basis of specific requirements. By optimizing the discharge parameters
the volume fraction of nitrogen oxides is increased from 4 180×10−6 to 12 097×10−6
an improvement of about 189%
while the energy consumption for nitrogen fixation is decreased from 4.6 MJ/mol to 2.4 MJ/mol
a reduction of about 50%
significantly enhancing the plasma nitrogen fixation efficiency.
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