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dc.contributor.authorXu, Shuchengen_US
dc.contributor.authorLin, M. C.en_US
dc.date.accessioned2014-12-08T15:10:15Z-
dc.date.available2014-12-08T15:10:15Z-
dc.date.issued2009-01-01en_US
dc.identifier.issn1540-7489en_US
dc.identifier.urihttp://dx.doi.org/10.1016/j.proci.2008.07.011en_US
dc.identifier.urihttp://hdl.handle.net/11536/7832-
dc.description.abstractThe kinetics and mechanisms of the reactions of cyanomidyl radical (HNCN) with oxygen atoms and molecules have been investigated by ab initio calculations with rate constant prediction. The doublet and quartet state potential energy surfaces (PESs) of the two reactions have been calculated by single-point calculations at the CCSD(T)/6-311+G(3df, 2p) level based on geometries optimized at the CCSD/6-311++G(d, p) level. The rate constants for various product channels of the two reactions in the temperature range of 300-3000 K are predicted by variational transition state and RRKM theories. The predicted total rate constants of the O((3)P) + HNCN reaction at 760 Torr Ar pressure can be represented by the expressions k(total) (O + HNCN) = 3.12 x 10(-10) x T(-0.05) exp (-37/T) cm(3) molecule(-1) s(-1) at T= 300-3000 K. The branching ratios of primary channels of the O((3)P) + HNCN are predicted: k(1) for producing the NO + CNH accounts for 0.72-0.64, k(2) + k(9) for producing the (3)NH + NCO accounts for 0.27-0.32, and k(6) for producing the CN + HNO accounts for 0.01-0.07 in the temperature range studied. Meanwhile, the predicted total rate constants of the O(2) + HNCN reaction at 760 Torr Ar pressure can be represented by the expression, k(total)(O(2) + HNCN) = 2.10 x 10(-16) x T(1.28)exp (-12200/T) cm(3) molecule(-1) s(-1) at T = 300-3000 K. The predicted branching ratio for k(11) + k(13) producing HO(2) + (3)NCN as the primary products accounts for 0.98-1.00 in the temperature range studied. (C) 2009 The Combustion Institute. Published by Elsevier Inc. All rights reserved.en_US
dc.language.isoen_USen_US
dc.titleAb initio chemical kinetics for the reactions of HNCN with O((3)P) and O(2)en_US
dc.typeArticleen_US
dc.identifier.doi10.1016/j.proci.2008.07.011en_US
dc.identifier.journalPROCEEDINGS OF THE COMBUSTION INSTITUTEen_US
dc.citation.volume32en_US
dc.citation.issueen_US
dc.citation.spage99en_US
dc.citation.epage106en_US
dc.contributor.department應用化學系分子科學碩博班zh_TW
dc.contributor.departmentInstitute of Molecular scienceen_US
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