14 research outputs found
Absolute Ultraviolet Absorption Spectrum of a Criegee Intermediate CH<sub>2</sub>OO
We
present the time-resolved UV absorption spectrum of the B̃
(<sup>1</sup>A′) ← X̃ (<sup>1</sup>A′)
electronic transition of formaldehyde oxide, CH<sub>2</sub>OO, produced
by the reaction of CH<sub>2</sub>I radicals with O<sub>2</sub>. In
contrast to its UV photodissociation action spectrum, the absorption
spectrum of formaldehyde oxide extends to longer wavelengths and exhibits
resolved vibrational structure on its low-energy side. Chemical kinetics
measurements of its reactivity establish the identity of the absorbing
species as CH<sub>2</sub>OO. Separate measurements of the initial
CH<sub>2</sub>I radical concentration allow a determination of the
absolute absorption cross section of CH<sub>2</sub>OO, with the value
at the peak of the absorption band, 355 nm, of σ<sub>abs</sub> = (3.6 ± 0.9) × 10<sup>–17</sup> cm<sup>2</sup>. The difference between the absorption and action spectra likely
arises from excitation to long-lived B̃ (<sup>1</sup>A′)
vibrational states that relax to lower electronic states by fluorescence
or nonradiative processes, rather than by photodissociation
A Combined Experimental and Theoretical Study of the Reaction OH + 2‑Butene in the 400–800 K Temperature Range
We
report a combined experimental and theoretical study of the
OH + cis-2-butene and OH + trans-2-butene reactions at combustion-relevant
conditions: pressures of 1–20 bar and temperatures of 400–800
K. We probe the OH radical time histories by laser-induced fluorescence
and analyze these experimental measurements with aid from time-dependent
master-equation calculations. Importantly, our investigation covers
a temperature range where experimental data on OH + alkene chemistry
in general are lacking, and interpretation of such data is challenging
due to the complexity of the competing reaction pathways. Guided by
theory, we unravel this complex behavior and determine the temperature-
and pressure-dependent rate coefficients for the three most important
OH + 2-butene reaction channels at our conditions: H abstraction,
OH addition to the double bond, and back-dissociation of the OH–butene
adduct
Resonance Stabilization Effects on Ketone Autoxidation: Isomer-Specific Cyclic Ether and Ketohydroperoxide Formation in the Low-Temperature (400–625 K) Oxidation of Diethyl Ketone
The pulsed photolytic chlorine-initiated
oxidation of diethyl ketone
[DEK; (CH<sub>3</sub>CH<sub>2</sub>)<sub>2</sub>CO], 2,2,4,4-<i>d</i><sub>4</sub>-DEK [<i>d</i><sub>4</sub>-DEK; (CH<sub>3</sub>CD<sub>2</sub>)<sub>2</sub>CO], and 1,1,1,5,5,5-<i>d</i><sub>6</sub>-DEK [<i>d</i><sub>6</sub>-DEK; (CD<sub>3</sub>CH<sub>2</sub>)<sub>2</sub>CO] is studied at 8 torr
and 1–2 atm and from 400–625 K. Cl atoms produced by
laser photolysis react with diethyl ketone to form either primary
(3-pentan-on-1-yl, R<sub>P</sub>) or secondary (3-pentan-on-2-yl,
R<sub>S</sub>) radicals, which in turn react with O<sub>2</sub>. Multiplexed
time-of-flight mass spectrometry, coupled to either a hydrogen discharge
lamp or tunable synchrotron photoionizing radiation, is used to detect
products as a function of mass, time, and photon energy. At 8 torr,
the nature of the chain propagating cyclic ether + OH channel changes
as a function of temperature. At 450 K, the production of OH is mainly
in conjunction with formation of 2,4-dimethyloxetan-3-one, resulting
from reaction of the resonance-stabilized secondary R<sub>S</sub> with
O<sub>2</sub>. In contrast, at 550 K and 8 torr, 2-methyl-tetrahydrofuran-3-one,
originating from oxidation of the primary radical (R<sub>P</sub>),
is observed as the dominant cyclic ether product. Formation of both
of these cyclic ether production channels proceeds via a resonance-stabilized
hydroperoxy alkyl (QOOH) intermediate. Little or no ketohydroperoxide
(KHP) is observed under the low-pressure conditions. At higher O<sub>2</sub> concentrations and higher pressures (1–2 atm), a strong
KHP signal appears as the temperature is increased above 450 K. Definitive
isomeric identification from measurements on the deuterated DEK isotopologues
indicates the favored pathway produces a γ-KHP via resonance-stabilized
alkyl, QOOH, and HOOPOOH radicals. Time-resolved measurements reveal
the KHP formation becomes faster and signal more intense upon increasing
temperature from 450 to 575 K before intensity drops significantly
at 625 K. The KHP time profile also shows a peak followed by a gradual
depletion for the extent of experiment. Several tertiary products
exhibit a slow accumulation in coincidence with the observed KHP decay.
These products can be associated with decomposition of KHP by β-scission
pathways or via isomerization of a γ-KHP into a cyclic peroxide
intermediate (Korcek mechanism). The oxidation of <i>d</i><sub>4</sub>-DEK, where kinetic isotope effects disfavor γ-KHP
formation, shows greatly reduced KHP formation and associated signatures
from KHP decomposition products
Quantification of Key Peroxy and Hydroperoxide Intermediates in the Low-Temperature Oxidation of Dimethyl Ether
Dimethyl ether (DME) oxidation is
a model chemical system
with
a small number of prototypical reaction intermediates that also has
practical importance for low-carbon transportation. Although it has
been studied experimentally and theoretically, ambiguity remains in
the relative importance of competing DME oxidation pathways in the
low-temperature autoignition regime. To focus on the primary reactions
in DME autoignition, we measured the time-resolved concentration of
five intermediates, CH3OCH2OO (ROO), OOCH2OCH2OOH (OOQOOH), HOOCH2OCHO (hydroperoxymethyl
formate, HPMF), CH2O, and CH3OCHO (methyl formate,
MF), from photolytically initiated experiments. We performed these
studies at P = 10 bar and T = 450–575
K, using a high-pressure photolysis reactor coupled to a time-of-flight
mass spectrometer with tunable vacuum-ultraviolet synchrotron ionization
at the Advanced Light Source. Our measurements reveal that the timescale
of ROO decay and product formation is much shorter than predicted
by current DME combustion models. The models also strongly underpredict
the observed yields of CH2O and MF and do not capture the
temperature dependence of OOQOOH and HPMF yields. Adding the ROO +
OH → RO + HO2 reaction to the chemical mechanism
(with a rate coefficient approximated from similar reactions) improves
the prediction of MF. Increasing the rate coefficients of ROO ↔
QOOH and QOOH + O2 ↔ OOQOOH reactions brings the
model predictions closer to experimental observations for OOQOOH and
HPMF, while increasing the rate coefficient for the QOOH →
2CH2O + OH reaction is needed to improve the predictions
of formaldehyde. To aid future quantification of DME oxidation intermediates
by photoionization mass spectrometry, we report experimentally determined
ionization cross-sections for ROO, OOQOOH, and HPMF
Quantification of Key Peroxy and Hydroperoxide Intermediates in the Low-Temperature Oxidation of Dimethyl Ether
Dimethyl ether (DME) oxidation is
a model chemical system
with
a small number of prototypical reaction intermediates that also has
practical importance for low-carbon transportation. Although it has
been studied experimentally and theoretically, ambiguity remains in
the relative importance of competing DME oxidation pathways in the
low-temperature autoignition regime. To focus on the primary reactions
in DME autoignition, we measured the time-resolved concentration of
five intermediates, CH3OCH2OO (ROO), OOCH2OCH2OOH (OOQOOH), HOOCH2OCHO (hydroperoxymethyl
formate, HPMF), CH2O, and CH3OCHO (methyl formate,
MF), from photolytically initiated experiments. We performed these
studies at P = 10 bar and T = 450–575
K, using a high-pressure photolysis reactor coupled to a time-of-flight
mass spectrometer with tunable vacuum-ultraviolet synchrotron ionization
at the Advanced Light Source. Our measurements reveal that the timescale
of ROO decay and product formation is much shorter than predicted
by current DME combustion models. The models also strongly underpredict
the observed yields of CH2O and MF and do not capture the
temperature dependence of OOQOOH and HPMF yields. Adding the ROO +
OH → RO + HO2 reaction to the chemical mechanism
(with a rate coefficient approximated from similar reactions) improves
the prediction of MF. Increasing the rate coefficients of ROO ↔
QOOH and QOOH + O2 ↔ OOQOOH reactions brings the
model predictions closer to experimental observations for OOQOOH and
HPMF, while increasing the rate coefficient for the QOOH →
2CH2O + OH reaction is needed to improve the predictions
of formaldehyde. To aid future quantification of DME oxidation intermediates
by photoionization mass spectrometry, we report experimentally determined
ionization cross-sections for ROO, OOQOOH, and HPMF
Quantification of Key Peroxy and Hydroperoxide Intermediates in the Low-Temperature Oxidation of Dimethyl Ether
Dimethyl ether (DME) oxidation is
a model chemical system
with
a small number of prototypical reaction intermediates that also has
practical importance for low-carbon transportation. Although it has
been studied experimentally and theoretically, ambiguity remains in
the relative importance of competing DME oxidation pathways in the
low-temperature autoignition regime. To focus on the primary reactions
in DME autoignition, we measured the time-resolved concentration of
five intermediates, CH3OCH2OO (ROO), OOCH2OCH2OOH (OOQOOH), HOOCH2OCHO (hydroperoxymethyl
formate, HPMF), CH2O, and CH3OCHO (methyl formate,
MF), from photolytically initiated experiments. We performed these
studies at P = 10 bar and T = 450–575
K, using a high-pressure photolysis reactor coupled to a time-of-flight
mass spectrometer with tunable vacuum-ultraviolet synchrotron ionization
at the Advanced Light Source. Our measurements reveal that the timescale
of ROO decay and product formation is much shorter than predicted
by current DME combustion models. The models also strongly underpredict
the observed yields of CH2O and MF and do not capture the
temperature dependence of OOQOOH and HPMF yields. Adding the ROO +
OH → RO + HO2 reaction to the chemical mechanism
(with a rate coefficient approximated from similar reactions) improves
the prediction of MF. Increasing the rate coefficients of ROO ↔
QOOH and QOOH + O2 ↔ OOQOOH reactions brings the
model predictions closer to experimental observations for OOQOOH and
HPMF, while increasing the rate coefficient for the QOOH →
2CH2O + OH reaction is needed to improve the predictions
of formaldehyde. To aid future quantification of DME oxidation intermediates
by photoionization mass spectrometry, we report experimentally determined
ionization cross-sections for ROO, OOQOOH, and HPMF
Low-Temperature Combustion Chemistry of <i>n-</i>Butanol: Principal Oxidation Pathways of Hydroxybutyl Radicals
Reactions
of hydroxybutyl radicals with O<sub>2</sub> were investigated by a
combination of quantum-chemical calculations and experimental measurements
of product formation. In pulsed-photolytic Cl-initiated oxidation
of <i>n</i>-butanol, the time-resolved and isomer-specific
product concentrations were probed using multiplexed tunable synchrotron
photoionization mass spectrometry (MPIMS). The interpretation of the
experimental data is underpinned by potential energy surfaces for
the reactions of O<sub>2</sub> with the four hydroxybutyl isomers
(1-hydroxybut-1-yl, 1-hydroxybut-2-yl, 4-hydroxybut-2-yl, and 4-hydroxybut-1-yl)
calculated at the CBS-QB3 and RQCISD(T)/cc-pV∞Z//B3LYP/6-311++G(d,p) levels of theory. The observed
product yields display substantial temperature dependence, arising
from a competition among three fundamental pathways: (1) stabilization
of hydroxybutylperoxy radicals, (2) bimolecular product formation
in the hydroxybutyl + O<sub>2</sub> reactions, and (3) decomposition
of hydroxybutyl radicals. The 1-hydroxybut-1-yl + O<sub>2</sub> reaction
is dominated by direct HO<sub>2</sub> elimination from the corresponding
peroxy radical forming butanal as the stable coproduct. The chemistry
of the other three hydroxybutylperoxy radical isomers mainly proceeds
via alcohol-specific internal H-atom abstractions involving the H
atom from either the −OH group or from the carbon attached
to the −OH group. We observe evidence of the recently reported
water elimination pathway (Welz et al. <i>J. Phys. Chem. Lett.</i> <b>2013</b>, <i>4</i> (3), 350–354) from
the 4-hydroxybut-2-yl + O<sub>2</sub> reaction, supporting its importance
in γ-hydroxyalkyl + O<sub>2</sub> reactions. Experiments using
the 1,1-<i>d</i><sub>2</sub> and 4,4,4-<i>d</i><sub>3</sub> isotopologues of <i>n</i>-butanol suggest
the presence of yet unexplored pathways to acetaldehyde
Pressure-Dependent Competition among Reaction Pathways from First- and Second‑O<sub>2</sub> Additions in the Low-Temperature Oxidation of Tetrahydrofuran
We
report a combined experimental and quantum chemistry study of
the initial reactions in low-temperature oxidation of tetrahydrofuran
(THF). Using synchrotron-based time-resolved VUV photoionization mass
spectrometry, we probe numerous transient intermediates and products
at <i>P</i> = 10–2000 Torr and <i>T</i> = 400–700 K. A key reaction sequence, revealed by our experiments,
is the conversion of THF-yl peroxy to hydroperoxy-THF-yl radicals
(QOOH), followed by a second O<sub>2</sub> addition and subsequent
decomposition to dihydrofuranyl hydroperoxide + HO<sub>2</sub> or
to γ-butyrolactone hydroperoxide + OH. The competition between
these two pathways affects the degree of radical chain-branching and
is likely of central importance in modeling the autoignition of THF.
We interpret our data with the aid of quantum chemical calculations
of the THF-yl + O<sub>2</sub> and QOOH + O<sub>2</sub> potential energy
surfaces. On the basis of our results, we propose a simplified THF
oxidation mechanism below 700 K, which involves the competition among
unimolecular decomposition and oxidation pathways of QOOH
C–H Bond Strengths and Acidities in Aromatic Systems: Effects of Nitrogen Incorporation in Mono-, Di-, and Triazines
The negative ion chemistry of five azine molecules has
been investigated
using the combined experimental techniques of negative ion photoelectron
spectroscopy to obtain electron affinities (EA) and tandem flowing
afterglow-selected ion tube (FA-SIFT) mass spectrometry to obtain
deprotonation enthalpies (Δ<sub>acid</sub><i>H</i><sub>298</sub>). The measured Δ<sub>acid</sub><i>H</i><sub>298</sub> for the most acidic site of each azine species is
combined with the EA of the corresponding radical in a thermochemical
cycle to determine the corresponding C–H bond dissociation
energy (BDE). The site-specific C–H BDE values of pyridine,
1,2-diazine, 1,3-diazine, 1,4-diazine, and 1,3,5-triazine are 110.4
± 2.0, 111.3 ± 0.7, 113.4 ± 0.7, 107.5 ± 0.4,
and 107.8 ± 0.7 kcal mol<sup>–1</sup>, respectively. The
application of complementary experimental methods, along with quantum
chemical calculations, to a series of nitrogen-substituted azines
sheds light on the influence of nitrogen atom substitution on the
strength of C–H bonds in six-membered rings
Unimolecular Kinetics of Stabilized CH<sub>3</sub>CHOO Criegee Intermediates: <i>syn</i>-CH<sub>3</sub>CHOO Decomposition and <i>anti</i>-CH<sub>3</sub>CHOO Isomerization
The kinetics of the unimolecular decomposition of the
stabilized
Criegee intermediate syn-CH3CHOO has been
investigated at temperatures between 297 and 331 K and pressures between
12 and 300 Torr using laser flash photolysis of CH3CHI2/O2/N2 gas mixtures coupled with time-resolved
broadband UV absorption spectroscopy. Fits to experimental results
using the Master Equation Solver for Multi-Energy well Reactions (MESMER)
indicate that the barrier height to decomposition is 67.2 ± 1.3
kJ mol–1 and that there is a strong tunneling component
to the decomposition reaction under atmospheric conditions. At 298
K and 760 Torr, MESMER simulations indicate a rate coefficient of
150–81+176 s–1 when tunneling effects are included but only
5–2+3 s–1 when tunneling is not considered in the model.
MESMER simulations were also performed for the unimolecular isomerization
of the stabilized Criegee intermediate anti-CH3CHOO to methyldioxirane, indicating a rate coefficient of
54–21+34 s–1 at 298 K and 760 Torr, which is not impacted
by tunneling effects. Expressions to describe the unimolecular kinetics
of syn- and anti-CH3CHOO
are provided for use in atmospheric models, and atmospheric implications
are discussed