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Is CH3NC isomerization an intrinsic non-RRKM unimolecular reaction

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dc.contributor.author Jayee, Bhumika en_US
dc.contributor.author MALPATHAK, SHREYAS en_US
dc.contributor.author Ma, Xinyou en_US
dc.contributor.author Hase, William L. en_US
dc.date.accessioned 2019-12-24T12:19:30Z
dc.date.available 2019-12-24T12:19:30Z
dc.date.issued 2019-11 en_US
dc.identifier.citation Journal of Chemical Physics, 151(18). en_US
dc.identifier.issn 0021-9606 en_US
dc.identifier.issn 1089-7690 en_US
dc.identifier.uri http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/4280
dc.identifier.uri https://doi.org/10.1063/1.5126805 en_US
dc.description.abstract Direct dynamics simulations, using B3LYP/6-311++G(2d,2p) theory, were used to study the unimolecular and intramolecular dynamics of vibrationally excited CH3NC. Microcanonical ensembles of CH3NC, excited with 150, 120, and 100 kcal/mol of vibrational energy, isomerized to CH3CN nonexponentially, indicative of intrinsic non-Rice-Ramsperger-Kassel-Marcus (RRKM) dynamics. The distribution of surviving CH3NC 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 CH3NC isomerization. Classical power spectra calculated for vibrationally excited CH3NC, at the experimental average energy of isomerizing molecules, show that the intramolecular dynamics of CH3NC are not chaotic and the C—N≡C and CH3 units are weakly coupled. The biexponential N(t)/N(0) at 100 kcal/mol is used as a model to study CH3NC → CH3CN isomerization with biexponential dynamics. The Hinshelwood-Lindemann rate constant kuni(ω,E) found from the biexponential N(t)/N(0) agrees with the Hinshelwood-Lindemann-RRKM kuni(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 kuni(ω,E) curves may be brought into agreement by scaling ω in the Hinshelwood-Lindemann-RRKM kuni(ω,E) by a collisional energy transfer efficiency factor βc. The interplay between the value of βc, for the actual intermolecular energy transfer, and the ways the treatment of the rotational quantum number K and nonexponential unimolecular dynamics affect βc suggests that the ability to fit an experimental kuni(ω,T) with Hinshelwood-Lindemann-RRKM theory does not identify a unimolecular reactant as an intrinsic RRKM molecule. en_US
dc.language.iso en en_US
dc.publisher AIP Publishing en_US
dc.subject Vibrational-Energy-Transfer en_US
dc.subject Chemical-Dynamics Simulations en_US
dc.subject Sn2 Nucleophilic-Substitution en_US
dc.subject Methyl Isocyanide en_US
dc.subject Rate Constants en_US
dc.subject Gateway Modes en_US
dc.subject Intramolecular Dynamics en_US
dc.subject Thermal-Isomerization en_US
dc.subject CD Overtones en_US
dc.subject Molecules en_US
dc.subject TOC-DEC-2019 en_US
dc.subject 2019 en_US
dc.title Is CH3NC isomerization an intrinsic non-RRKM unimolecular reaction en_US
dc.type Article en_US
dc.contributor.department Dept. of Chemistry en_US
dc.identifier.sourcetitle Journal of Chemical Physics en_US
dc.publication.originofpublisher Foreign en_US


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