研究目的
To analyze the emission from microwave-induced argon plasma promoted by activated cokes during non-catalytic reduction of nitric oxide at atmospheric pressure, focusing on spectroscopic measurements and plasma dynamic behavior to understand the reaction mechanisms and enhance NO reduction.
研究成果
The study revealed that emission in the 388 nm band is due to Ar(II) ions enhanced by interactions during NO reduction, with plasma temperatures reaching up to 40,000 K indicating non-equilibrium conditions. Dynamic plasma behavior was observed, and NO reduction conversion correlated with the plasma area ratio, suggesting potential for improving reactivity through enhanced plasma exposure.
研究不足
The detailed mechanism of plasma interaction and NO reduction is too complicated to fully clarify. The study is fundamental and not directly applicable to industrial processes without further optimization. Gas analysis for N2 yield was difficult due to low concentrations and atmospheric interference.
1:Experimental Design and Method Selection:
The study used spectroscopic measurements and high-speed camera imaging to analyze microwave-induced plasma in a reactor with activated cokes. Spectroscopic analysis involved high-resolution measurements of emission spectra, and plasma temperatures were determined using Boltzmann plots.
2:Sample Selection and Data Sources:
Activated cokes (commercial adsorbent from coal) were used, packed in a quartz reactor tube. Test gases included Ar, N2, and Ar + NO mixtures.
3:List of Experimental Equipment and Materials:
Equipment included a microwave generator (magnetron), spectroscope, CCD camera, high-speed camera, digital camera, NOx analyzer, quartz reactor tube, and activated cokes.
4:Experimental Procedures and Operational Workflow:
Gas was supplied at
5:0 L/min, microwave power varied from 100 W to 500 W. Spectra were measured after plasma ignition, and plasma behavior was observed with cameras. NO concentration in exit gas was measured. Data Analysis Methods:
Spectral intensities were analyzed to determine plasma temperatures via Boltzmann plots. Image analysis involved calculating the ratio of plasma area to reactor cross-section.
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