Energy partitioning and reaction dynamics in the chemiluminescent channel of the reaction: HS + O3 → HSO* + O2

1984 ◽  
Vol 110 (2) ◽  
pp. 183-190 ◽  
Author(s):  
D.J.W. Kendall ◽  
J.J.A. O'Brien ◽  
J.J. Sloan ◽  
R.Glen Macdonald
2006 ◽  
Vol 110 (9) ◽  
pp. 3017-3027 ◽  
Author(s):  
Wenfang Hu ◽  
György Lendvay ◽  
Diego Troya ◽  
George C. Schatz ◽  
Jon P. Camden ◽  
...  

2020 ◽  
Vol 71 (1) ◽  
pp. 289-313 ◽  
Author(s):  
Bhumika Jayee ◽  
William L. Hase

Nonstatistical dynamics is important for many chemical reactions. The Rice-Ramsperger-Kassel-Marcus (RRKM) theory of unimolecular kinetics assumes a reactant molecule maintains a statistical microcanonical ensemble of vibrational states during its dissociation so that its unimolecular dynamics are time independent. Such dynamics results when the reactant's atomic motion is chaotic or irregular. Intrinsic non-RRKM dynamics occurs when part of the reactant's phase space consists of quasiperiodic/regular motion and a bottleneck exists, so that the unimolecular rate constant is time dependent. Nonrandom excitation of a molecule may result in short-time apparent non-RRKM dynamics. For rotational activation, the 2J + 1 K levels for a particular J may be highly mixed, making K an active degree of freedom, or K may be a good quantum number and an adiabatic degree of freedom. Nonstatistical dynamics is often important for bimolecular reactions and their intermediates and for product-energy partitioning of bimolecular and unimolecular reactions. Post–transition state dynamics is often highly complex and nonstatistical.


2010 ◽  
Vol 315 (2) ◽  
pp. 135-147 ◽  
Author(s):  
Tatsuo Matsushima ◽  
Kosuke Shobatake

1991 ◽  
Vol 174 (Part_2) ◽  
pp. 225-225
Author(s):  
Wolfgang Schirmer

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