2015
DOI: 10.1109/tps.2015.2403280
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Atmospheric Pressure 2.45-GHz Microwave Helium Plasma

Abstract: A waveguide-based microwave plasma system was built using a resonant cavity and a quartz tube. 2.45 GHz 850 W magnetron was used to obtain helium discharge without an igniter. The temporal images of discharge were recorded on microsecond time scales using an intensified charge-coupled device camera. The excitation temperature was calculated as 3385 K using the helium lines, which were obtained from emission spectrum of the discharge. The gas temperature was measured as 1208 K by a thermocouple.

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Cited by 15 publications
(4 citation statements)
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(18 reference statements)
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“…The spectroscopic data related to the wavelengths of excited atoms and ions were confirmed via the NIST atomic database [28]. By adding argon gas, the contributed wavelengths of helium [27] for the estimation of electron temperature weakened; therefore, the wavelengths of argon [12] were used at the flow rate of 400 to 2000 sccm.…”
Section: Measurements Of Gas Temperaturementioning
confidence: 99%
See 1 more Smart Citation
“…The spectroscopic data related to the wavelengths of excited atoms and ions were confirmed via the NIST atomic database [28]. By adding argon gas, the contributed wavelengths of helium [27] for the estimation of electron temperature weakened; therefore, the wavelengths of argon [12] were used at the flow rate of 400 to 2000 sccm.…”
Section: Measurements Of Gas Temperaturementioning
confidence: 99%
“…The production of hydroxyl might be explained by two possible different mechanisms The Boltzmann plot equation is assumed to be ln(Iλ/gA) = −E/kT e + constant, where I is the measured intensity obtained by OES, λ is the selected wavelength associated with helium and argon gases, g is the statistical weight, A is the transition probability, E is the excitation energy corresponding to the selected wavelengths, k is Boltzmann constant, and T e is electron temperature. The selected wavelengths of atomic emission lines related to argon and helium gases were obtained from references [12,27] to estimate the electron temperature based on the Boltzmann plot. The spectroscopic data related to the wavelengths of excited atoms and ions were confirmed via the NIST atomic database [28].…”
Section: Measurements Of Electron Density and Electron Temperaturementioning
confidence: 99%
“…The various techniques to measure gas temperature include optical emission spectroscopy (OES) [1,[6][7][8][9][10][11][12][13][14][15], infrared thermometry [1,[16][17][18], millimetre wave interferometry [19], Schlieren [1,5], Rayleigh scattering [20,21], thermocouple [1,11,22,23], and fibre optic based thermometry [24,25]. These have been applied to a varying degree in different plasma systems including plasma torch [15,26,27], dielectric barrier discharge [1,7,14,18,19], plasma jet [5,8,9,16,20,24,27,28], gliding arc discharge, [2,17,25] and glow discharge [21].…”
Section: Introductionmentioning
confidence: 99%
“…lines derived from the OES measurement could be used for the determination of electron temperature. But, for a plasma in non-LTE this method could give an approximation of excitation temperature (T exc ) [42,43]. Intensities from several excited helium lines (471.31 nm, 492.19 nm, 501.57 nm, 587.56 nm, 667.80 nm, 706.52 nm and 728.13 nm) were included in the model assuming a Boltzmann distribution of the population of the atomic level as [42]: ln…”
Section: Electron Densitymentioning
confidence: 99%