Back to Search Start Over

Is CH 3 NC isomerization an intrinsic non-RRKM unimolecular reaction?

Authors :
Jayee B
Malpathak S
Ma X
Hase WL
Source :
The Journal of chemical physics [J Chem Phys] 2019 Nov 14; Vol. 151 (18), pp. 184110.
Publication Year :
2019

Abstract

Direct dynamics simulations, using B3LYP/6-311++G(2d,2p) theory, were used to study the unimolecular and intramolecular dynamics of vibrationally excited CH <subscript>3</subscript> NC. Microcanonical ensembles of CH <subscript>3</subscript> NC, excited with 150, 120, and 100 kcal/mol of vibrational energy, isomerized to CH <subscript>3</subscript> CN nonexponentially, indicative of intrinsic non-Rice-Ramsperger-Kassel-Marcus (RRKM) dynamics. The distribution of surviving CH <subscript>3</subscript> NC molecules vs time, i.e., N(t)/N(0), was described by two separate functions, valid above and below a time limit, a single exponential for the former and a biexponential for the latter. The dynamics for the short-time component are consistent with a separable phase space model. The importance of this component decreases with vibrational energy and may be unimportant for energies relevant to experimental studies of CH <subscript>3</subscript> NC isomerization. Classical power spectra calculated for vibrationally excited CH <subscript>3</subscript> NC, at the experimental average energy of isomerizing molecules, show that the intramolecular dynamics of CH <subscript>3</subscript> NC are not chaotic and the C-N≡C and CH <subscript>3</subscript> units are weakly coupled. The biexponential N(t)/N(0) at 100 kcal/mol is used as a model to study CH <subscript>3</subscript> NC → CH <subscript>3</subscript> CN isomerization with biexponential dynamics. The Hinshelwood-Lindemann rate constant k <subscript>uni</subscript> (ω,E) found from the biexponential N(t)/N(0) agrees with the Hinshelwood-Lindemann-RRKM k <subscript>uni</subscript> (ω,E) at the high and low pressure limits, but is lower at intermediate pressures. As found from previous work [S. Malpathak and W. L. Hase, J. Phys. Chem. A 123, 1923 (2019)], the two k <subscript>uni</subscript> (ω,E) curves may be brought into agreement by scaling ω in the Hinshelwood-Lindemann-RRKM k <subscript>uni</subscript> (ω,E) by a collisional energy transfer efficiency factor β <subscript>c</subscript> . The interplay between the value of β <subscript>c</subscript> , for the actual intermolecular energy transfer, and the ways the treatment of the rotational quantum number K and nonexponential unimolecular dynamics affect β <subscript>c</subscript> suggests that the ability to fit an experimental k <subscript>uni</subscript> (ω,T) with Hinshelwood-Lindemann-RRKM theory does not identify a unimolecular reactant as an intrinsic RRKM molecule.

Details

Language :
English
ISSN :
1089-7690
Volume :
151
Issue :
18
Database :
MEDLINE
Journal :
The Journal of chemical physics
Publication Type :
Academic Journal
Accession number :
31731854
Full Text :
https://doi.org/10.1063/1.5126805