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Investigation of Water-Vapor Plasma Excited by Microwaves as Ultraviolet Light Source

机译:微波作为紫外光源激发水蒸气等离子体的研究

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摘要

The potential of using water-vapor plasmas excited by microwaves as a ultraviolet (UV) light source has been investigated by using various pressures and input powers. The UV irradiation power increased and saturated at a pressure range dependent on the input power. On the other hand, other visible and infrared emissions corresponding to four atomic lines, i.e., the Balmer series of hydrogen at 486.1 nm (Hβ) and 656.3 nm (Hα) and oxygen atoms at 777.2 and 844.6 nm, were clearly decreased with an increase in the total gas pressure. It was found that pressures (1.4–2.0 kPa) near the saturated water-vapor pressure were found to give the most intense UV irradiation. With a vapor pressure of 1.6 kPa and a total microwave power of 300 W, the power density of UV (Γuv) was measured to be 10.5 μW · cm−2 at a distance of 30 cm from the center of the discharge tube as measured through an optical viewing port on the cavity discharge applicator. This value for (Γuv) is comparable to that for a mercury lamp. However, the (ηuv) efficiency was estimated to be considerably lower than that of a mercury lamp.
机译:通过使用各种压力和输入功率,已经研究了使用由微波激发的水蒸气等离子体作为紫外线(UV)光源的潜力。 UV照射功率在取决于输入功率的压力范围内增加并达到饱和。另一方面,与四个原子谱线相对应的其他可见光和红外光发射明显增加,分别是486.1 nm(Hβ)和656.3 nm(Hα)的巴尔默级数氢和777.2和844.6 nm的氧原子总气压。结果发现,接近饱和水蒸气压力的压力(1.4–2.0 kPa)产生最强烈的紫外线照射。在蒸气压为1.6 kPa且总微波功率为300 W的情况下,通过测量,在距放电管中心30 cm处,UV(Γuv)的功率密度为10.5μW·cm-2。腔体排放施药器上的光学观察口。 (Γuv)的该值与水银灯的相当。但是,估计(ηuv)效率明显低于水银灯的效率。

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