微型微波等离子体喷灯应用中的等离子体辅助燃烧

Pub Date : 2005-06-20 DOI:10.1109/PLASMA.2005.359524
K. Hemawan, S. Zuo, C. Romel, T. Grotjohn, I. Wichman, E. Case, J. Asmussen
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引用次数: 0

摘要

只提供摘要形式。设计了一种紧凑的微波等离子体火炬,并对其在等离子体燃烧模式和等离子体辅助燃烧模式下的运行进行了实验评估。火炬的设计是轻的,在大气压力下操作,火炬放电直径小于1毫米。焊枪的潜在应用是材料合成、材料切割和焊接以及各种表面处理。利用微波功率改变燃烧过程,研究了火炬在烃类气体与氧气或空气燃烧的燃烧模式下的运行情况。本研究的目的是量化当微波功率被应用于产生或加强放电时燃烧过程中的变化。该火炬采用外径12毫米的开放式同轴结构,放电点位于中心导体的尖端,直径为5毫米。2.45 GHz的微波功率以10到100瓦的功率水平耦合到火炬应用器中。在大气压力下形成放电,其中原料气流经位于施药器中心导体末端的200-500 μ m直径的喷嘴孔。研究了两种喷嘴结构,包括水冷黄铜喷嘴和陶瓷喷嘴。微波等离子体炬用多种原料气混合物进行了实验评估,包括氩气、氩气与氢气的混合物、氩气与氮气、甲烷和氧气的混合物,以及选定的其他碳氢化合物气体与氧气和空气的混合物。这种火炬保持放电在广泛的流动范围内,从扩散流动平缓的表面处理到接近超音速的高速流动。进行的诊断测量包括:(1)通过光学发射光谱(OES)测量的气体温度,(2)放电功率密度,(3)放电体积和大小。这些测量是根据吸收的微波功率、气体流速和气体混合物成分进行的。通过使用空间分辨的OES测量,确定了放电的温度分布。仅使用等离子体操作模式(即氩气)的吸收微波功率为10-30瓦时,放电尺寸直径为0.4-0.5毫米,喷嘴直径为0.25毫米时,放电长度为2-4毫米。当火炬在等离子体辅助燃烧模式下工作时,随着微波功率的施加,火焰(放电)的体积和强度增加。将给出量化微波功率对火焰影响的数据。
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Plasma-assisted combustion in a miniature microwave plasma torch applicator
Summary form only given. A compact microwave plasma torch has been designed and experimentally evaluated for operation in both plasma-only and plasma-assisted combustion modes. The torch is designed to be light and to operate at atmospheric pressure with a torch discharge size of less than 1 mm in diameter. The potential applications of the torch are for materials synthesis, material cutting and welding, and various surface treatments. The operation of the torch in a combustion mode with hydrocarbon gases burning with oxygen or air is investigated with microwave power applied to modify the combustion process. The objective of this investigation is to quantify the changes in the combustion process as microwave power is applied to create or intensify the discharge. This torch employs an open ended coaxial structure of 12 mm outer diameter with the discharge located at the tip of the center conductor that is 5 mm in diameter. Microwave power at 2.45 GHz is coupled into the torch applicator at power levels of 10's to 100's of watts. The discharge is formed at atmospheric pressure where the feed gas flows through a nozzle hole of 200-500 mum diameter located at the end of the applicator center conductor. Two nozzle configurations studied include a water-cooled brass nozzle and a ceramic nozzle. The microwave plasma torch is experimentally evaluated with a variety of feed gas mixtures including argon, mixtures of argon with hydrogen, argon with nitrogen, methane and oxygen, and selected other hydrocarbon gases mixed with oxygen and air. This torch maintains discharges over a wide range of flows from diffusional flow for gentle surface processing to high velocity flow approaching supersonic velocities. Diagnostic measurements performed include (1) gas temperature measured by optical emission spectroscopy (OES), (2) discharge power densities and, (3) discharge volume and size. These measurements are performed versus absorbed microwave power, gas flow rate and gas mixture composition. By using spatially resolved OES measurements, the temperature profile of the discharge is determined. The discharge size for absorbed microwave powers of 10-30 watts using a plasma-only mode of operation (i.e. argon) is 0.4-0.5 mm in diameter and 2-4 mm long for a nozzle diameter of 0.25 mm. When the torch is operated in a plasma-assisted combustion mode the flame (discharge) volume and intensity increase as the microwave power is applied to the flame. Data quantifying the influence of microwave power on the flame will be presented.
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