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大气压下氩气中微波诱导等离子体的建模。

Modeling of microwave-induced plasma in argon at atmospheric pressure.

作者信息

Baeva M, Bösel A, Ehlbeck J, Loffhagen D

机构信息

Leibniz Institute for Plasma Science and Technology, INP Greifswald, Germany.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2012 May;85(5 Pt 2):056404. doi: 10.1103/PhysRevE.85.056404. Epub 2012 May 15.

DOI:10.1103/PhysRevE.85.056404
PMID:23004876
Abstract

A two-dimensional model of microwave-induced plasma (field frequency 2.45 GHz) in argon at atmospheric pressure is presented. The model describes in a self-consistent manner the gas flow and heat transfer, the in-coupling of the microwave energy into the plasma, and the reaction kinetics relevant to high-pressure argon plasma including the contribution of molecular ion species. The model provides the gas and electron temperature distributions, the electron, ion, and excited state number densities, and the power deposited into the plasma for given gas flow rate and temperature at the inlet, and input power of the incoming TEM microwave. For flow rate and absorbed microwave power typical for analytical applications (200-400 ml/min and 20 W), the plasma is far from thermodynamic equilibrium. The gas temperature reaches values above 2000 K in the plasma region, while the electron temperature is about 1 eV. The electron density reaches a maximum value of about 4 × 10(21) m(-3). The balance of the charged particles is essentially controlled by the kinetics of the molecular ions. For temperatures above 1200 K, quasineutrality of the plasma is provided by the atomic ions, and below 1200 K the molecular ion density exceeds the atomic ion density and a contraction of the discharge is observed. Comparison with experimental data is presented which demonstrates good quantitative and qualitative agreement.

摘要

本文提出了一个二维大气压氩气中微波诱导等离子体(场频率2.45GHz)模型。该模型以自洽的方式描述了气体流动与传热、微波能量与等离子体的耦合,以及与高压氩等离子体相关的反应动力学,包括分子离子种类的贡献。对于给定的入口气体流速和温度以及入射TEM微波的输入功率,该模型可给出气体和电子温度分布、电子、离子和激发态数密度,以及沉积到等离子体中的功率。对于分析应用中的典型流速和吸收微波功率(200 - 400ml/min和20W),等离子体远非热力学平衡态。在等离子体区域,气体温度达到2000K以上,而电子温度约为1eV。电子密度最大值约为4×10(21)m(-3)。带电粒子的平衡主要由分子离子的动力学控制。对于温度高于1200K的情况,等离子体的准中性由原子离子提供;而在1200K以下,分子离子密度超过原子离子密度,观察到放电收缩现象。文中给出了与实验数据的比较,结果表明在定量和定性方面都有良好的一致性。

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