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Measurements of spatially resolved electron number densities and modes temperatures using optical emission spectroscopy of atmospheric pressure microplasma jet

机译:使用大气压微等离子体射流的发射光谱测量空间分辨的电子数密度和模式温度

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The electrical gas discharge parameters of direct-current non-thermal microplasma jet in Ar-2%H2 flow at open atmospheric air was investigated by using spatially resolved optical emission spectroscopy (OES). The jet was confined from microhollow of tungsten-carbide (?500 μm inner diameter) to a molybdenum foil. Despite its small volume, the atmospheric pressure microplasma jet provides a range of power densities, from low to ?10 ~(12) W m ~(-3) generated either in rare gases or in molecular gases. A high resolution spectrometer (Jobin-Yvon, Czerny-Turner model THR1000, resolution of 0.001 nm, with focal length of 1.0 m and numerical aperture of 0.13-f/7.5) was used to allow registration of OH (A ~2S ~+, ν = 0 → X ~2π, ν,ν = 0) rotational bands at 306.357 nm, Ar I 603.213 nm line and N _2 (C ~3π _u, ν = 0 → B ~3π _g, ν = 0) second positive system with the band head at 337.13 nm in order to estimate the rotational temperature from the cathode sheath of the plasma jet to the anode. For currents ranging from 20 to 100 mA and for a particular excited levels, the excitation temperature was measured in the negative glow region either from a Boltzmann plot of Ar I 4p-4s and 5p-4s transitions of excited argon or using the Mo I (from 440 to 450 nm) two-lines method of excited Mo atoms sputtered from the cathode surface, giving 24 000 K (100 mA at 100 μm) and 7000 K (20 mA at 500 μm from the cathode). From the N _2 (C ~3pi; _u, nu; = 0 → B ~3π _g, ν = 0) rotational transition the rotational temperature along the positive column was estimated. The vibrational temperature of the bulk plasma (1400 to 4500 K) was estimated for a current varying from 20 to 120 mA using the N ~2 second positive system with δν =-2. Using the broadening of Hβ Balmer line it was possible to estimate the electron number density of the negative glow (10 ~(14) to 10 ~(15) cm ~(-3)) as a function of the current.
机译:利用空间分辨光发射光谱法研究了在大气中Ar-2%H2气流中直流非热微等离子体射流的电气体放电参数。射流从碳化钨的微空心(内径约为500μm)限制在钼箔中。尽管其体积很小,但常压微等离子体射流提供的功率密度范围很低,从稀有气体或分子气体中产生的功率密度低至?10〜(12)W m〜(-3)。使用高分辨率光谱仪(Jobin-Yvon,Czerny-Turner型号THR1000,分辨率为0.001 nm,焦距为1.0 m,数值孔径为0.13-f / 7.5)来记录OH(A〜2S〜+, ν= 0→X〜2π,ν,ν= 0)在306.357 nm处的旋转带,Ar I 603.213 nm线和N _2(C〜3π_u,ν= 0→B〜3π_g,ν= 0)第二正系统带头在337.13 nm处,以估计从等离子流阴极鞘到阳极的旋转温度。对于20至100 mA的电流以及特定的激发水平,可以通过Ar I 4p-4s和5p-4s跃迁氩的Boltzmann图或使用Mo I在负辉光区域中测量激发温度。从440到450 nm)的两线方法,从阴极表面溅射出激发的Mo原子,得到24000 K(100μm为100 mA)和7000 K(500μm为距阴极20 mA)。从N _2(C〜3pi; _u,nu; = 0→B〜3π_g,ν= 0)旋转跃迁,可以估算出沿正柱的旋转温度。使用δν= -2的N〜2第二正系统,对于20至120 mA的电流变化,估计了整体等离子体的振动温度(1400至4500 K)。使用Hβ巴尔默线的加宽,可以估计负辉光的电子数密度(10〜(14)至10〜(15)cm〜(-3))作为电流的函数。

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