A dual‐level ab initio and hybrid density functional theory dynamics study on the unimolecular decomposition reaction C2H5O → CH2O + CH3

We present a direct ab initio and hybrid density functional theory dynamics study of the thermal rate constants of the unimolecular decomposition reaction of C2H5O → CH2O + CH3 at a high‐pressure limit. MPW1K/6‐31+G(d,p), MP2/6‐31+G(d,p), and MP2(full)/6‐31G(d) methods were employed to optimize the geometries of all stationary points and to calculate the minimum energy path (MEP). The energies of all the stationary points were refined at a series of multicoefficient and multilevel methods. Among all methods, the QCISD(T)/aug‐cc‐pVTZ energies are in good agreement with the available experimental data. The rate constants were evaluated based on the energetics from the QCISD(T)/aug‐cc‐pVTZ//MPW1K/6‐31+G(d,p) level of theory using both microcanonical variational transition state theory (μVT) and RRKM theory with the Eckart tunneling correction in the temperature range of 300–2500 K. The calculated rate constants at the QCISD(T)/aug‐cc‐pVTZ/MPW1K/6‐31+G(d,p) level of theory are in good consistent with experimental data. The fitted three‐parameter Arrhenius expression from the μVT/Eckart rate constants in the temperature range 200–2500 K is k = 2.52 × 1012T0.41e(−8894.0/T) s−1. The falloff curves of pressure‐dependent rate constants are performed using master‐equation method within the temperature range of 391–471 K. The calculated results are in good agreement with the available experimental data. © 2004 Wiley Periodicals, Inc. J Comput Chem 2: 218–226, 2003

[1]  Thanh N. Truong,et al.  TheRate: Program for ab initio direct dynamics calculations of thermal and vibrational‐state‐selected rate constants , 1998 .

[2]  Donald G. Truhlar,et al.  Improved canonical and microcanonical variational transition state theory calculations for a polyatomic reaction: OH+H2→H2O+H , 1985 .

[3]  Martin Head-Gordon,et al.  Quadratic configuration interaction. A general technique for determining electron correlation energies , 1987 .

[4]  Thanh N. Truong,et al.  Branching Ratio and Pressure Dependent Rate Constants of Multichannel Unimolecular Decomposition of Gas-Phase α-HMX: An Ab Initio Dynamics Study† , 2001 .

[5]  G. Lendvay,et al.  INTRAMOLECULAR H ATOM TRANSFER REACTIONS IN ALKYL RADICALS AND THE RING STRAIN ENERGY IN THE TRANSITION STRUCTURE , 1996 .

[6]  Stuart A. Rice,et al.  Theory of Unimolecular Reactions , 1960 .

[7]  Donald G. Truhlar,et al.  EXACT TUNNELING CALCULATIONS. , 1971 .

[8]  S. Benson,et al.  Arrhenius parameters for the alkoxy radical decomposition reactions , 1981 .

[9]  M. Jacox Matrix isolation study of the infrared spectrum and structure of the CH3 free radical , 1977 .

[10]  B. Viskolcz,et al.  Reactions of C2H5Radicals with O, O3, and NO3: Decomposition Pathways of the Intermediate C2H5O Radical , 1999 .

[11]  O. Nielsen,et al.  Role of Excited CF3CFHO Radicals in the Atmospheric Chemistry of HFC-134a , 1996 .

[12]  Krishnan Raghavachari,et al.  Gaussian-3 theory using reduced Mo/ller-Plesset order , 1999 .

[13]  S. Dóbé,et al.  Kinetics of the reaction between methoxyl radicals and hydrogen atoms , 1991 .

[14]  B. Viskolcz,et al.  The thermal unimolecular decomposition rate constants of ethoxy radicals , 1999 .

[15]  Donald G. Truhlar,et al.  Improved treatment of threshold contributions in variational transition-state theory , 1980 .

[16]  L. Batt The gas‐phase decomposition of alkoxy radicals , 1979 .

[17]  P. Devolder Atmospheric fate of small alkoxy radicals: recent experimental and theoretical advances , 2003 .

[18]  Donald G. Truhlar,et al.  Adiabatic connection for kinetics , 2000 .

[19]  L. Curtiss,et al.  Gaussian-3 (G3) theory for molecules containing first and second-row atoms , 1998 .

[20]  M. Fajardo,et al.  Matrix isolation spectroscopy of laser ablated carbon species in Ne, D2, and H2 matrices , 1997 .

[21]  B. C. Garrett,et al.  Current status of transition-state theory , 1983 .

[22]  J. L. Duncan,et al.  The ground-state average and equilibrium structures of formaldehyde and ethylene , 1974 .

[23]  James A. Miller,et al.  The reaction between ethyl and molecular oxygen II: Further analysis , 2001 .

[24]  F. Lovas,et al.  Microwave Spectra of Molecules of Astrophysical Interest: II Methylenimine , 1973 .

[25]  Donald G. Truhlar,et al.  How Well Can Hybrid Density Functional Methods Predict Transition State Geometries and Barrier Heights , 2001 .

[26]  Sean C. Smith,et al.  Theory of Unimolecular and Recombination Reactions , 1990 .

[27]  D. Truhlar,et al.  How Should We Calculate Transition State Geometries for Radical Reactions? The Effect of Spin Contamination on the Prediction of Geometries for Open-Shell Saddle Points , 2000 .

[28]  J. Uhlenbusch,et al.  Determination of the absolute Raman cross section of methyl , 1996 .

[29]  Michael J. Pilling,et al.  Evaluated Kinetic Data for Combustion Modelling , 1992 .

[30]  B. C. Garrett,et al.  Generalized transition state theory. Quantum effects for collinear reactions of hydrogen molecules and isotopically substituted hydrogen molecules , 1979 .

[31]  R. Atkinson Gas-phase tropospheric chemistry of organic compounds: a review , 1990 .

[32]  W. C. Martin,et al.  Energy levels of magnesium, Mg I through Mg XII , 1980 .

[33]  R. Nesbet Algorithm for Diagonalization of Large Matrices , 1965 .

[34]  H. Bernhard Schlegel,et al.  An improved algorithm for reaction path following , 1989 .

[35]  D. Truhlar,et al.  Ab initio transition state theory calculations of the reaction rate for OH+CH4→H2O+CH3 , 1990 .

[36]  Jan M.L. Martin,et al.  Benchmark ab Initio Energy Profiles for the Gas-Phase SN2 Reactions Y- + CH3X → CH3Y + X- (X,Y = F,Cl,Br). Validation of Hybrid DFT Methods , 2000 .

[37]  B. J. Tyler,et al.  Unimolecular Reactions , 1966, Nature.

[38]  M. Gordon,et al.  From Force Fields to Dynamics: Classical and Quantal Paths , 1990, Science.

[39]  Takehiko Shimanouchi,et al.  Tables of molecular vibrational frequencies. Consolidated volume II , 1972 .

[40]  W. Carter,et al.  Atmospheric chemistry of alkanes , 1985 .

[41]  T. Truong,et al.  Kinetics of Hydrogen Abstraction Reaction Class H + H−C(sp3): First-Principles Predictions Using the Reaction Class Transition State Theory , 2003 .

[42]  T. Wallington,et al.  Laboratory and theoretical study of the oxy radicals in the OH- and Cl-initiated oxidation of ethene , 1998 .

[43]  W. Hase Some Recent Advances and Remaining Questions Regarding Unimolecular Rate Theory , 1998 .

[44]  D. Golden,et al.  Photochemical smog. Rate parameter estimates and computer simulations , 1977 .

[45]  B. C. Garrett,et al.  SEMICLASSICAL TUNNELING CALCULATIONS , 1979 .

[46]  W. D. Allen,et al.  Fragmentation path for hydrogen atom dissociation from methoxy radical , 2002 .

[47]  W. Carter,et al.  Reactions of alkoxy radicals under atmospheric conditions: The relative importance of decomposition versus reaction with O2 , 1991 .