Measurements of the bimolecular rate constants for S + O2 ? SO + O and CS2 + O2 ? CS + SO2 at high temperatures

1986 ◽  
Vol 18 (8) ◽  
pp. 871-884 ◽  
Author(s):  
Ko Saito ◽  
Yuji Ueda ◽  
Reiko Ito ◽  
Terumitsu Kakumoto ◽  
Akira Imamura
2018 ◽  
Vol 17 (06) ◽  
pp. 1850040
Author(s):  
Qian Li ◽  
Li Yao ◽  
S. H. Lin

The unimolecular dissociation rate constants of the dehydration of Glycerol to Glycidol were calculated at the MP2/6–311G(d,p) level using the Rice–Ramsperger–Kassel–Marcus (RRKM) theory. The anharmonic effect of the reactions was examined by comparing the rate constants at temperatures (700–3000[Formula: see text]K) of the canonical case and total energies (25654–53089[Formula: see text]cm[Formula: see text]) of the microcanonical system. The calculations showed that high temperatures are required for the reaction to proceed. As the temperatures and total energies increased, the rate of reactions increased. However, the growth rate of the unimolecular dissociation rate constants was high and slower both in the canonical and microcanonical systems. Comparative analysis showed that the anharmonic effect was most significant for the reaction [Formula: see text] and least significant for the reaction [Formula: see text]. The anharmonic effect became more significant as the temperatures and total energies increased. Compared with the microcanonical situation, the anharmonic effect of the canonical system was more pronounced.


1990 ◽  
Vol 86 (9) ◽  
pp. 1539 ◽  
Author(s):  
A. John Elliot ◽  
David R. McCracken ◽  
George V. Buxton ◽  
Nicholas D. Wood

1982 ◽  
Vol 86 (5) ◽  
pp. 700-703 ◽  
Author(s):  
Patricia M. Borrell ◽  
Peter Borrell ◽  
Kevin R. Grant ◽  
Michael D. Pedley

The excited states of oxygen, O 2 ( 1 Δ g ) and O 2 ( 1 Σ g + ), generated in a microwave discharge, were shock heated in order to study their reactions at temperatures in the range 650-1650 K. The increase in the dimol emission (634 nm) from O 2 ( 1 Δ g ) behind the shock front is consistent with the simple collisional model for the production of the emission; the rate of quenching of O 2 ( 1 Δ g ) by O 2 is too slow to measure at high temperatures with the technique. The emission from O 2 ( 1 Σ g + ) increases because of the shock compression and then is further enhanced by a displacement in the steady state concentration which is maintained by the two reactions pooling: 2O 2 ( 1 Δ g )->O 2 ( 1 Σ g + )+O 2 ( 3 Σ g - ) k p ; quenching: O 2 ( 1 Σ g + )+M->O 2 ( 3 Σ g - or 1 Δ g )+M; k q M . The relaxation to the enhanced level of emission permits k M q to be measured directly and then k p is calculated from the enhanced steady state emission level and k M q . There is no evidence for direct, collision induced! enhancement of the emission from O 2 ( 1 Σ g + ). Curved Arrhenius plots of the rate constants were found; some values are given in table 2. The results appear to indicate that in each case there are two mechanisms operating; one involving short range forces, and the other, long range forces or a collision complex. An evaluation is given of the discharge flow-shock tube technique as a method for determining rate constants at high temperatures.


Sign in / Sign up

Export Citation Format

Share Document