Qf. Chen et Jm. Goodings, CHEMICAL-KINETICS OF YTTRIUM IONIZATION IN H-2-O-2-N-2 FLAMES, International journal of mass spectrometry and ion processes, 176(1-2), 1998, pp. 1-12
Citations number
26
Categorie Soggetti
Spectroscopy,"Physics, Atomic, Molecular & Chemical
Trace amounts (less than or equal to 10(-6) mol fraction) of yttrium w
ere introduced into six H-2-O-2-N-2 flames in the temperature range 18
20-2400 K at atmospheric pressure. Metallic ions were observed by samp
ling the flames through a nozzle into a mass spectrometer, and were me
asured as profiles of ion concentration vs. distance (i.e. time) along
the flame axis. The ions observed conform to a series YO+ . nH(2)O (n
= 0-3); YO+ is barely detectable, Y(OH)(2)(+) with n = 1 is the domin
ant ion, and the higher hydrates are produced by cooling that occurs d
uring sampling. The major yttrium neutral species are the oxide-hydrox
ide OYOH (> 80%) and the oxide YO (< 20%). By the addition of 0.25 mol
% of CH4 and a trace of potassium, it was possible to boost the ioniz
ation level appropriately to make electron-ion recombination of Y(OH)(
2)(+) the dominant process; values of the recombination coefficient (9
.7 +/- 1.5)T-2.3 +/- 0.6 cm(3) molecule(-1) s(-1) were obtained. A rad
ical species such as H in these flames can overshoot its equilibrium c
oncentration by a factor gamma of 100 or more in the reaction zone but
gamma decays downstream towards equilibrium. Neutral OYOH and YO, who
se concentrations depend on gamma, are linked by the balanced reaction
YO + H2O = OYOH + H having an equilibrium constant K = exp(-49,000/RT
). This leads to a bond energy value D-o(OY-OH) = 449 +/- 20 kT mol(-1
). Analysis of the ion profiles as a function of gamma is helpful in a
scertaining the ion formation processes. Yttrium ions are produced by
the chemi-ionization reaction of OYOH with H; because the ionization e
nergy of YO is low, a small contribution (< 1%) might arise from colli
sional (thermal) ionization of YO. The rate constant for chemi-ionizat
ion was found to be (2.7 +/- 0.8) X 10(-12) exp(-22452/T) cm(3) molecu
le(-1) s(-1). This rate constant should be regarded as a lower limit b
ecause a fraction of the total yttrium, presumably small, may be prese
nt in these flames as solid particles. (Int J Mass Spectrom 176 (1998)
1-12) (C) 1998 Elsevier Science B.V.