Availability and reactivity of N2(v) for NH3 synthesis by plasma catalysis

Brian N Bayer, Sai Raskar, Igor V Adamovich, Peter J Bruggeman, Aditya Bhan
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Abstract

Production of vibrationally excited N2 (N2(v)) in atmospheric pressure nonthermal plasma and loss of N2(v) by gas-phase reactions and reactions on catalytic surfaces are analyzed to examine the role of N2(v) in NH3 formation by plasma catalysis. Vibrational state-to-state kinetic models complemented with molecular beam mass spectrometry (MBMS) measurements demonstrate that N2(v> 0) is produced with densities 100× greater than the density of N radicals by a radiofrequency atmospheric pressure plasma jet. The experimentally measured loss of N2(v) corresponds with a state-to-state kinetic model that describes loss of N2(v) by surface-mediated vibrational relaxation without consideration of reactions that convert N2(v) to NH3 over the catalyst surface. Rate constants for vibrational relaxation of N2(v) on catalyst surfaces exceed upper bounds on proposed rate constants for NH3 formation reactions from N2(v) over Fe when v < 9, Ni when v < 18, and Ag when v < 39, which indicates that only higher vibrational levels can possibly contribute to catalytic NH3 formation faster than they undergo vibrational relaxation on the surface. Densities of N2(v> 8), vibrational levels that can possibly react over Fe to form NH3 faster than they undergo vibrational relaxation, are less than or similar to N densities at the inlet of the catalyst bed and measured NH3 formation for the investigated conditions in this work, while densities of N2(v> 17) and N2(v> 38) are orders of magnitude below the N density at the inlet of the catalyst bed and the measured NH3 formation. The loss of N2(v) by vibrational relaxation on the surface limits the ability of N2(v) to contribute to catalytic NH3 formation and explains why N2(v) does not produce NH3 in quantities that are comparable to NH3 formation from N even though N2(v > 0) is more abundantly produced by the plasma.
利用等离子催化合成 NH3 时 N2(v) 的可用性和反应性
分析了常压非热等离子体中振动激发的 N2(N2(v))的产生以及通过气相反应和催化表面反应损失的 N2(v),以研究 N2(v)在等离子体催化形成 NH3 中的作用。振荡态-态动力学模型辅以分子束质谱(MBMS)测量结果表明,射频大气压等离子体射流产生的 N2(v> 0) 密度比 N 自由基密度大 100 倍。实验测得的 N2(v) 损失与状态到状态动力学模型相符,该模型描述了 N2(v) 通过表面介导的振动弛豫损失,而没有考虑催化剂表面将 N2(v) 转化为 NH3 的反应。催化剂表面 N2(v) 振动弛豫的速率常数超过了所提出的 N2(v) 在铁表面(v < 9 时)、镍表面(v < 18 时)和银表面(v < 39 时)形成 NH3 反应的速率常数上限,这表明只有较高的振动水平才有可能以比它们在表面振动弛豫更快的速度促进催化 NH3 的形成。N2(v>8)的密度(有可能与铁发生反应生成 NH3 的振动水平)小于或类似于催化剂床层入口处的 N 密度和本研究中调查条件下测得的 NH3 生成量,而 N2(v> 17) 和 N2(v> 38) 的密度则比催化剂床层入口处的 N 密度和测得的 NH3 生成量低几个数量级。表面振动弛豫造成的 N2(v) 损失限制了 N2(v) 催化 NH3 生成的能力,这也解释了为什么 N2(v) 生成的 NH3 数量无法与 N 生成的 NH3 数量相提并论,即使等离子体生成的 N2(v> 0) 数量更多。
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