62 research outputs found
Low-Temperature Mechanisms for the Formation of Substituted Azanaphthalenes through Consecutive CN and C<sub>2</sub>H Additions to Styrene and <i>N</i>‑Methylenebenzenamine: A Theoretical Study
Ab initio G3(MP2,CC)/B3LYP/6-311G**
calculations of potential energy
surfaces (PESs) for the reactions of cyano and ethynyl radicals with
styrene and N-methylenebenzenamine have been performed
to investigate a possible formation mechanism of the prototype nitrogen-containing
polycyclic aromatic compounds: (substituted) 1- and 2-azanaphthalenes.
The computed PESs and molecular parameters have been used for RRKM
and RRKM-Master Equation calculations of reaction rate constants and
product branching ratios under single-collision conditions and at
pressures from 3 to 10–6 mbar and temperatures of
90–200 K relevant to the organic aerosol formation regions
in the stratosphere of a Saturn’s moon Titan. The results show
that ethynyl-substituted 1- and 2-azanaphthalenes can be produced
by consecutive CN and C2H additions to styrene or by two
C2H additions to N-methylenebenzenamine.
All CN and C2H radical addition complexes are formed in
the entrance channels without barriers, and the reactions are computed
to be exothermic, with all intermediates and transition states along
the favorable pathways residing lower in energy than the respective
initial reactants. The reactions are completed by dissociation of
chemically activated radical intermediates via H losses, so that collisional
stabilization of the intermediates is not required to form the final
products. These features make the proposed mechanism viable even at
very low temperatures and under single-collision conditions and especially
significant for astrochemical environments. In Titan’s stratosphere,
collisional stabilization of the initial CN + styrene reaction adducts
may be significant, but substantial amounts of 2-vinylbenzonitrile
and 2-ethynyl-N-methylenebenzenamine can still be
produced and then react with C2H to form substituted azanaphthalenes
On the Mechanism of Soot Nucleation. IV. Molecular Growth of the Flattened E‑Bridge
Rotationally excited
dimerization of aromatic moieties, a mechanism
proposed recently to explain the initial steps of soot particle inception
in combustion and pyrolysis of hydrocarbons, produces a molecular
structure, termed E-bridge, combining the two aromatics via five-membered
aromatic rings sharing a common bond. The present study investigates
a hydrogen-mediated addition of acetylene to the fused five-membered
ring part of the E-bridge forming a seven-membered ring. The carried
out quantum-mechanical and rate theoretical calculations indicate
the plausibility of such capping reactions, and kinetic Monte Carlo
simulations demonstrate their frequent occurrence. The capping frequency,
however, is limited by “splitting” the fused five-membered
bridge due to five-membered ring migration. A similar migration of
edge seven-membered rings is shown to be also rapid but short, as
their encounter with five-membered rings converts them both into six-membered
rings
Reactions of C<sub>2</sub>H with 1- and 2-Butynes: An Ab Initio/RRKM Study of the Reaction Mechanism and Product Branching Ratios
Ab initio CCSD(T)/cc-pVTZ(CBS)//B3LYP/6-311G** calculations of the C6H7 potential energy surface are combined with RRKM calculations of reaction rate constants and product branching ratios to investigate the mechanism and product distribution in the C2H + 1-butyne/2-butyne reactions. 2-Ethynyl-1,3-butadiene (C6H6) + H and ethynylallene (C5H4) + CH3 are predicted to be the major products of the C2H + 1-butyne reaction. The reaction is initiated by barrierless ethynyl additions to the acetylenic C atoms in 1-butyne and the product branching ratios depend on collision energy and the direction of the initial C2H attack. The 2-ethynyl-1,3-butadiene + H products are favored by the central C2H addition to 1-butyne, whereas ethynylallene + CH3 are preferred for the terminal C2H addition. A relatively minor product favored at higher collision energies is diacetylene + C2H5. Three other acyclic C6H6 isomers, including 1,3-hexadiene-5-yne, 3,4-hexadiene-1-yne, and 1,3-hexadiyne, can be formed as less important products, but the production of the cyclic C6H6 species, fulvene, and dimethylenecyclobut-1-ene (DMCB), is predicted to be negligible. The qualitative disagreement with the recently measured experimental product distribution of C6H6 isomers is attributed to a possible role of the secondary 2-ethynyl-1,3-butadiene + H reaction, which may generate fulvene as a significant product. Also, the photoionization energy curve assigned to DMCB in experiment may originate from vibrationally excited 2-ethynyl-1,3-butadiene molecules. For the C2H + 2-butyne reaction, the calculations predict the C5H4 isomer methyldiacetylene + CH3 to be the dominant product, whereas very minor products include the C6H6 isomers 1,1-ethynylmethylallene and 2-ethynyl-1,3-butadiene
Theoretical Study of the Reaction Mechanism and Kinetics of the Phenyl + Allyl and Related Benzyl + Vinyl Associations
Potential
energy surfaces for the allyl + phenyl and benzyl + vinyl
barrierless radical association reactions have been studied at the
CCSD(T)-F12/cc-pVTZ-f12//B3LYP/6-311G** level of theory. Variable
reaction coordinate transition state theory (VRC-TST) has been employed
to evaluate high-pressure limit rate constants for the barrierless
channels. Then, Rice–Ramsperger–Kassel–Marcus
master equation (RRKM-ME) calculations have been performed to assess
phenomenological rate constants and product branching ratios of various
reaction channels at different temperatures and pressures. The initial
step of both radical association reactions produces 3-phenylpropene
which can further dissociate into a variety of bimolecular products
including the indene precursor
1-phenylallyl + H. The results showed that at typical combustion conditions
the collisional stabilization of 3-phenylpropene dominates both the
phenyl + allyl and benzyl + vinyl reactions at temperatures below
1000 K and remains important at high pressures up to 2500 K. The main
bimolecular products of the two reactions at high temperatures are
predicted to be benzyl + vinyl and phenyl + allyl, respectively. The
well-skipping mechanism to form 1-phenylallyl directly in the allyl
+ phenyl and benzyl + vinyl reactions appeared to be not significant,
however, the reactions can provide some contributions into the formation
of the indene precursor via the 3-phenylpropene stabilization/dissociation
sequence and most of all, via the formation of 3-phenylpropene itself,
which then can undergo H-abstraction by available radicals to produce
1-phenylallyl. The allyl + phenyl reaction can also contribute to
the formation of two-ring PAH by producing benzyl radical at high
temperatures, either by the well-skipping or stabilization/dissociation
mechanisms; in turn, benzyl can readily react with acetylene or propargyl
radical to form indene or naphthalene precursors, respectively. Rate
expressions for all important reaction channels in a broad range of
temperatures and pressures have been generated for kinetic modeling
Theoretical Study on the Reaction Mechanism of CO<sub>2</sub> with Mg
Ab initio QCISD(T)/6-311+G(3df)//MP2/6-31+G(d) calculations of potential energy surface for the reaction
of Mg atoms with CO2 show that re-forming of carbon dioxide to carbon monoxide can be significantly
enhanced in the presence of Mg atoms. The overall endothermicity of the Mg + CO2 → MgO + CO reaction
is calculated to be about 66 kcal/mol, almost twice lower than the energy needed for spin-forbidden unimolecular
decomposition of CO2 to CO + O(3P). The Mg + CO2 reaction is spin-allowed and the barrier, 68.8 kcal/mol, is greatly reduced as compared to the barrier for the unimolecular decomposition, 131 kcal/mol. The
reaction proceeds via the MgOCO cyclic intermediate which lies 14.3 kcal/mol higher in energy than the
reactants and stabilized with respect to Mg + CO2 by a barrier of 5.9 kcal/mol. The catalytic role of Mg
atoms for re-forming of CO2 to CO is discussed. The reverse MgO + CO → Mg + CO2 reaction is highly
exothermic and has a barrier of 2.8 kcal/mol indicating that magnesium oxide can be rapidly reduced by
carbon monoxide producing Mg atoms and carbon dioxide. Highly accurate full valence active space MRCI
calculations with extrapolation to the complete basis set allowed us to propose a new value for the standard
heat of formation of MgO in the gas phase, 31.4−31.9 and 33.5−34.0 kcal/mol for ΔHf°(0 K) and ΔHf°(298
K), respectively. The result is 20 kcal/mol higher than the present recommended value and new experimental
measurements of thermochemical data for gaseous MgO are suggested
Reaction Mechanism of N<sub>2</sub>/H<sub>2</sub> Conversion to NH<sub>3</sub>: A Theoretical Study
Ab initio G2M(MP2)//MP2/6-31G** calculations have been performed to study the molecular and radical
chain reaction mechanisms of nitrogen hydrogenation through sequential additions of three H2 molecules to
N2 producing NH3 + NH3. All reaction steps of the molecular mechanism are shown to be slow owing to
high barriers for the molecular hydrogen additions. The three-center 1,1-H2 additions are significantly more
preferable as compared to the four-center 1,2-additions. The most favorable reaction pathway involves the
steps N2 + H2 → TS1a → NNH2, NNH2 + H2 → TS3a → H2NNH2, H2NNH2 → TS4 → HNNH3, and
HNNH3 + H2 → TS5 → NH3 + NH3, with the barriers calculated as 125.2, 30.7, 60.5, and 24.6 kcal/mol,
respectively. The addition of the first molecular hydrogen is thus the rate-determining stage of nitrogen
hydrogenation. The formation of hydrazine can be facilitated by a spontaneous reaction of two cis-HNNH
molecules by the dihydrogen transfer mechanism. The radical chain mechanism includes the N2 + H → N2H,
N2H + H2 → HNNH + H, HNNH + H → N2H3, N2H3 + H2 → H2NNH2 + H, H2NNH2 + H → NH2 + NH3,
and NH2 + H2 → NH3 + H sequential reactions with the barriers of 17.1, 41.6, 6.4, 29.1, 10.7, and 10.6
kcal/mol, respectively. Nitrogen hydrogenation can be catalyzed by H atoms with the barrier for the slowest
reaction step decreasing from 125 to 42 kcal/mol. The reaction of two NH(3Σ-) radicals is predicted to be
fast and to form N2 + H2 with high exothermicity. The reaction of two NH2 radicals can produce NNH2 +
H2 with exothermicity of 19.8 kcal/mol and a barrier of 10.9 kcal/mol relative to the reactants, or NH3 +
NH(3Σ-), through a barrierless, 14.3 kcal/mol exothermic, but spin-forbidden channel. We also report rate
constants and equilibrium constants for all considered reactions calculated using the transition state theory
and ab initio energies and molecular parameters, which can be employed for kinetic modeling of chemical
processes involving nitrogen- and hydrogen-containing substances
Theoretical Study on the Reaction Mechanism of Nickel Atoms with Carbon Dioxide
Ab initio and density functional calculations of the potential energy surfaces for the Ni + CO2 → NiO + CO
reaction in the lowest triplet and singlet electronic states have been carried out at the B3LYP/6-31G*, B3LYP/6-311G*, B3LYP/6-311+G(3df), CCSD(T)/6-311G*, and CCSD(T)/6-311+G(3df) theoretical levels. The
reaction is calculated to preferentially occur in the triplet state and to proceed by the formation of a cyclic
four-member ring C2v-symmetric NiOCO intermediate (t-cyc) that lies ∼19 kcal/mol above the reactants.
The barrier for the initial reaction step is about 23 kcal/mol. From t-cyc the reaction continues via transition
state t-TS2 toward the linear t-CONiO complex. The latter is stabilized by ∼10 kcal/mol with respect to the
products, NiO (3Σ-) + CO, and can dissociate producing them without exit barrier. The highest barrier at the
reaction pathway, about 53 kcal/mol, occurs at t-TS2. The reverse NiO (3Σ-) + CO reaction yielding Ni
atoms and CO2 with exothermicity of 36 kcal/mol is shown to have a barrier of 15 kcal/mol relative to the
reactants occurring at the second reaction step. On this basis, nickel oxide is expected to be less efficient for
oxidizing CO to CO2 than the oxides of alkaline earth metals. Reduction of CO2 to CO can be significantly
enhanced in the presence of Ni atoms due to much lower endothermicity (36−37 kcal/mol) and activation
barrier (∼53 kca/mol) for the t-Ni + CO2 → NiO (3Σ-) + CO reaction as compared to those for the
unimolecular decomposition of carbon dioxide. The accuracies of different theoretical methods for calculations
of the reaction energies have been compared
Activation of Methane by Neutral Transition Metal Oxides (ScO, NiO, and PdO): A Theoretical Study
Density functional B3LYP calculations have been employed to investigate potential energy surfaces for the
reactions of scandium, nickel, and palladium oxides with methane. The results show that NiO and PdO are
reactive toward methane and can form molecular complexes with CH4 bound by 9−10 kcal/mol without a
barrier. At elevated temperatures, the dominant reaction channel is direct abstraction of a hydrogen atom by
the oxides from CH4 with a barrier of ∼16 kcal/mol leading to MOH (M = Ni, Pd) and free methyl radical.
A minor reaction channel is an insertion into a C−H bond to produce CH3MOH molecules via transition
states lying 19−20 kcal/mol above the initial reactants. For instance, for PdO, the rate constant of the hydrogen
abstraction channel evaluated using the transition state theory for the 300−1000 K temperature range,
kmethyl = 7.12 × 10-11 exp(−17 329/RT) cm3 s-1 molecule-1, is 2−3 orders of magnitude higher than the
insertion rate constant and the branching ratio for the PdOH + CH3 products is 98−99%. The preferable
channel of dissociation of CH3NiOH is a cleavage of the Ni−C bond leading to the radical NiOH + CH3
products without an exit barrier, while CH3PdOH is more likely to undergo 1,2-CH3 migration to produce a
PdCH3OH complex and eventually Pd plus methanol. PdOH and CH3 can recombine producing CH3PdOH
and isomerization, and dissociation of this molecule results in further transformation of methyl radical into
methanol. However, the NiOH + CH3 reaction is expected only to produce CH3NiOH or to restore the initial
reactants, NiO + CH4. ScO is not reactive with respect to methane at low and ambient temperatures. At
elevated temperatures, the ScO + CH4 reaction can proceed via a barrier of 22.4 kcal/mol to form a CH3ScOH
molecule with exothermicity of 9.8 kcal/mol. CH3ScOH is not likely to decompose to the methyl radical and
ScOH because this process is 58.9 kcal/mol endothermic
Theoretical Investigation of the Mechanism and Product Branching Ratios of the Reactions of Cyano Radical with 1- and 2‑Butyne and 1,2-Butadiene
Ab initio CCSD(T)/cc-pVTZ(CBS)//B3LYP/6-311g(d,p) calculations
of the C<sub>5</sub>H<sub>6</sub>N potential energy surface have been
performed to investigate the reaction mechanism of cyano radical (CN)
with C<sub>4</sub>H<sub>6</sub> isomers 1- and 2-butyne and 1,2-butadiene.
They were followed by RRKM calculations of the reaction rate constants
and product branching ratios under single-collision conditions in
the 0–5 kcal/mol collision energy range. With the assumption
of equal probabilities of the barrierless terminal and central addition
of the cyano radical to 1-butyne, 2-cyano-1,3-butadiene + H, and cyanoallene
+ CH<sub>3</sub> are predicted to be the major reaction products with
a branching ratio of ∼2:1. The terminal CN addition to C<sup>1</sup> favors the formation of cyanoallene + CH<sub>3</sub>, whereas
the central CN addition to C<sup>2</sup> enhances the formation of
2-cyano-1,3-butadiene + H. For the CN + 2-butyne reaction, the dominant
product is calculated to be 1-cyano-prop-1-yne + CH<sub>3</sub>, and
the CH<sub>3</sub> loss occurs directly from the initial adduct formed
by the barrierless CN addition to either of the two acetylenic carbon
atoms. A small amount of the H loss product, 3-cyano-1,2-butadiene
(1-cyano-1-methylallene), can be also formed as was observed in earlier
crossed molecular beam experiments. Three different products are predicted
for the CN + 1,2-butadiene reaction, which also occurs without entrance
barriers. If various initial complexes formed by the CN addition to
C<sup>1</sup>, C<sup>2</sup>, C<sup>3</sup>, or to the CC
double bonds in 1,2-butadiene are produced in the entrance channel
with equal probabilities, the dominating product (70–60%) is
2-cyano-1,3-butadiene + H, and the other significant products include
1-cyano-prop-3-yne + CH<sub>3</sub> (19–25%) favored by the
initial CN addition to C<sup>1</sup> and cyanoallene + CH<sub>3</sub> (11–15%) preferred for the CN addition to C<sup>3</sup>.
The H abstraction HCN + C<sub>4</sub>H<sub>5</sub> products may also
be formed either from the initial CN addition adducts through a CN
roaming mechanism or via certain trajectories directly from the initial
reactants, but their yield is not expected to be significant, at least
at low temperatures. The energetics, mechanisms, and product branching
ratios of the cyano radical reactions with various C<sub>4</sub>H<sub>6</sub> isomers and their analogous isoelectronic C<sub>2</sub>H
+ C<sub>4</sub>H<sub>6</sub> reactions have been summarized and compared
Theoretical Study of TiO-Catalyzed Hydrogenation of Carbon Dioxide to Formic Acid
Density functional B3LYP/6-311+G(3df,2p)//B3LYP/6-31G(d,p) calculations have been performed for the
potential energy surface of the CO2/H2/TiO system. The results demonstrate that titanium oxide can serve as
a catalyst for the gas-phase hydrogenation of carbon dioxide to formic acid. The most favorable reaction
pathways are CO2 + H2 + TiO(3Δ) → H2 + η2-CO2−TiO → TS2 → η2-CO2−HTiOH → TS3 → OC(H)OTiOH
→ TS4 → cyc-HCO2TiOH → TS5 → cis-HOC(H)OTiO → cis-HCOOH + TiO(3Δ) and (starting from the
OC(H)OTiOH intermediate) OC(H)OTiOH → TS6 → trans-HC(O)O(H)TiO → trans-HCOOH + TiO(3Δ).
In these mechanisms, the highest relative energies with respect to the initial reactants are found for the final
products, 7.4 and 11.0 kcal/mol for the trans and cis conformers of formic acid, respectively, and all transition
states have lower energies. Therefore, in the gas phase, titanium oxide can be an efficient catalyst; the activation
energy for the TiO-catalyzed hydrogenation of CO2 coincides with its endothermicity. However, the highest
barriers for individual reaction steps are lowered to 60.1 and 54.5 kcal/mol, respectively, as compared to 73.8
kcal/mol for the uncatalyzed CO2 + H2 → HCOOH reaction, indicating that in the condensed phase TiO
would not be a particularly efficient catalyst
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