Vibrational population distribution of ground state BaO formed by the reaction Ba + O2

1976 ◽  
Vol 39 (3) ◽  
pp. 454-456 ◽  
Author(s):  
Michael A. Revelli ◽  
Brian G. Wicke ◽  
David O. Harris
1986 ◽  
Vol 6 (1) ◽  
pp. 15-35 ◽  
Author(s):  
Bernard Bourguignon ◽  
Joelle Rostas ◽  
Guy Taieb ◽  
Mohammed-Ali Gargoura ◽  
June McCombie

The internal state distribution of MgO(a3Π) formed from Mg(3P) + O2 and N2O reactions was determined from a reanalysis of the laser induced fluorescence spectra of the d3Δ - a3Π system previously published by Dagdigian. The MgO(a3Π) state formed in the reaction with O2 has a quasi-Boltzmann distribution. In the N2O reaction the rotational excitation is much greater and the vibrational population distribution is inverted with a maximum at v = 2 - 3. The a3Π rovibrational population distributions are compared with those of the X1∑+ ground state. The dynamics of these reactions are discussed on the basis of earlier ab-initio calculations and experimental data.


1994 ◽  
Vol 72 (3) ◽  
pp. 714-720
Author(s):  
Chris Carruthers ◽  
Heshel Teitelbaum

The master equation is solved numerically for the time dependence of the vibrational level populations of HCl (treated as a simple harmonic oscillator) during the bimolecular exchange reaction, Br + HCl → HBr + Cl, taking into account the competition between reaction and vibrational equilibration subject to Landau–Teller T–V excitation. Strong deviations from Boltzmann distributions are found. A wide range of reactant concentrations, diluent concentrations and temperatures were explored. It was found that no significant reaction occurs before the establishment of a steady vibrational population distribution, confirming that the rate coefficient for non-equilibrium bimolecular exchange reactions can be determined from a simple analytical steady state treatment (J. Chem. Soc. Faraday Trans. 87, 229 (1991)). The rate of an isolated elementary bimolecular reaction, A + BC → AB + C, under non-equilibrium conditions can deviate seriously from the standard expression, Keq [A][BC], and is better given by the law[Formula: see text]where [R] is the concentration of the collisional equilibrator, R, and a and g are constants depending only on temperature. This generalized rate law describes not only the initial rate but also the rate all the way up to completion, in the absence of the reverse reaction.


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