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Statements

Subject Item
n2:RIV%2F61389021%3A_____%2F12%3A00384027%21RIV13-GA0-61389021
rdf:type
skos:Concept n8:Vysledek
dcterms:description
Předneseno na:12th European Plasma Conference (12th High-Tech Plasma Processes conference, HTPP-12),Bologna,IT,24.-29.06.2012, PS1.11 Population distributions of argon atomic and ionic excited states in the supersonic part of a plasma jet expanding from the H2O-Ar dc arc torch into a chamber maintained at a pressure of 10 kPa have been studied by optical emission spectroscopy. The excitation temperatures are obtained from ArI (13.1-15.3 eV) and ArII Boltzmann (19.2-22.5 eV) diagrams. The ionization temperature is obtained from the intensity ratio of argon ionic and atomic lines, using electron number density calculated from the Stark broadening of hydrogen Hß line and Saha equation. A systematic difference in the total excitation temperature between both argon systems is found, with the ionic excitation temperature being significantly higher and close to the ionization temperature. The Boltzmann plots also reveal that the population distribution within a given electronic configuration Předneseno na:12th European Plasma Conference (12th High-Tech Plasma Processes conference, HTPP-12),Bologna,IT,24.-29.06.2012, PS1.11 Population distributions of argon atomic and ionic excited states in the supersonic part of a plasma jet expanding from the H2O-Ar dc arc torch into a chamber maintained at a pressure of 10 kPa have been studied by optical emission spectroscopy. The excitation temperatures are obtained from ArI (13.1-15.3 eV) and ArII Boltzmann (19.2-22.5 eV) diagrams. The ionization temperature is obtained from the intensity ratio of argon ionic and atomic lines, using electron number density calculated from the Stark broadening of hydrogen Hß line and Saha equation. A systematic difference in the total excitation temperature between both argon systems is found, with the ionic excitation temperature being significantly higher and close to the ionization temperature. The Boltzmann plots also reveal that the population distribution within a given electronic configuration
dcterms:title
Spectroscopic investigation of multiple Boltzmann distributions of various atomic and ionic states in an expanding H2O-Ar dc arc jet Spectroscopic investigation of multiple Boltzmann distributions of various atomic and ionic states in an expanding H2O-Ar dc arc jet
skos:prefLabel
Spectroscopic investigation of multiple Boltzmann distributions of various atomic and ionic states in an expanding H2O-Ar dc arc jet Spectroscopic investigation of multiple Boltzmann distributions of various atomic and ionic states in an expanding H2O-Ar dc arc jet
skos:notation
RIV/61389021:_____/12:00384027!RIV13-GA0-61389021
n8:predkladatel
n10:ico%3A61389021
n4:aktivita
n7:P n7:Z
n4:aktivity
P(GAP205/11/2070), Z(AV0Z20430508)
n4:dodaniDat
n15:2013
n4:domaciTvurceVysledku
Mašláni, Alan n12:1743163
n4:druhVysledku
n18:O
n4:duvernostUdaju
n14:S
n4:entitaPredkladatele
n9:predkladatel
n4:idSjednocenehoVysledku
170374
n4:idVysledku
RIV/61389021:_____/12:00384027
n4:jazykVysledku
n16:eng
n4:klicovaSlova
expanding plasma jet; optical emission spectroscopy; Boltzmann distribution
n4:klicoveSlovo
n6:expanding%20plasma%20jet n6:Boltzmann%20distribution n6:optical%20emission%20spectroscopy
n4:kontrolniKodProRIV
[11F9DA4181A5]
n4:obor
n17:BL
n4:pocetDomacichTvurcuVysledku
2
n4:pocetTvurcuVysledku
2
n4:projekt
n5:GAP205%2F11%2F2070
n4:rokUplatneniVysledku
n15:2012
n4:tvurceVysledku
Sember, Viktor Mašláni, Alan
n4:zamer
n11:AV0Z20430508