6 research outputs found
Butadiene and Heterodienes Revisited
Surprising features in a recently
published high-level calculation
of the rotational profile of butadiene led us to compare butadiene
with a set of 17 heterodienes. The rotational profiles for this large
group of compounds varied widely, thereby possessing a high information
content. These data were subjected to a Fourier analysis yielding
1- through 6-fold terms: the one-fold terms represent the change in
steric energy on going from 180° to 0°, while the changes
in the 2-fold terms correspond to the expected change in π-delocalization
energy with structure; the 3-fold terms were significant and found
to be linearly correlated to the average of the atomic charges of
the atoms at the central single bond of the <i>cis</i>-forms,
but their origins are still not clear; we propose a novel 1,4 π-interactions that may account for this phenomenon. The 4-fold terms
were at times comparable in magnitude to the 3-fold terms but overall
appeared to mainly modify the 3-fold terms slightly without introducing
any qualitatively new features. The 5- and 6-fold terms were negligible
Laser-Induced Fluorescence Study of the S<sub>1</sub> State of Doubly-Substituted <sup>13</sup>C Acetylene and Harmonic Force Field Determination
In
the first half of this study, rotational and vibrational constants
of six Franck–Condon bright vibrational levels of S<sub>1</sub> doubly-substituted <sup>13</sup>C acetylene are determined from
laser-induced fluorescence spectra and an updated geometry of the
trans conformer of S<sub>1</sub> acetylene is obtained. In the second
half, we determine the quadratic force field of S<sub>1</sub> acetylene
on the basis of the harmonic frequencies of four isotopologues of
acetylene. The effects of both diagonal and off-diagonal <i>x</i><sub><i>ij</i></sub> anharmonicities are removed from the
input harmonic frequencies. Results from both experimental and theoretical
studies of various isotopologues of acetylene (including those from
the first half of this paper) are used to obtain a set of force constants
that agrees well with ab initio calculations. Our set of force constants
for S<sub>1</sub> acetylene is an improvement over previous work by
Tobiason et al., which did not include off-diagonal anharmonicities
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Isomerization and Fragmentation of Cyclohexanone in a Heated Micro-Reactor
The thermal decomposition of cyclohexanone
(C<sub>6</sub>H<sub>10</sub>î—»O) has been studied in a set of
flash-pyrolysis microreactors.
Decomposition of the ketone was observed when dilute samples of C<sub>6</sub>H<sub>10</sub>î—»O were heated to 1200 K in a continuous
flow microreactor. Pyrolysis products were detected and identified
by tunable VUV photoionization mass spectroscopy and by photoionization
appearance thresholds. Complementary product identification was provided
by matrix infrared absorption spectroscopy. Pyrolysis pressures were
roughly 100 Torr, and contact times with the microreactors were roughly
100 μs. Thermal cracking of cyclohexanone appeared to result
from a variety of competing pathways, all of which open roughly simultaneously.
Isomerization of cyclohexanone to the enol, cyclohexen-1-ol (C<sub>6</sub>H<sub>9</sub>OH), is followed by retro-Diels–Alder
cleavage to CH<sub>2</sub>î—»CH<sub>2</sub> and CH<sub>2</sub>î—»CÂ(OH)–CHî—»CH<sub>2</sub>. Further isomerization
of CH<sub>2</sub>î—»CÂ(OH)–CHî—»CH<sub>2</sub> to
methyl vinyl ketone (CH<sub>3</sub>CO–CHCH<sub>2</sub>, MVK) was also observed. Photoionization spectra identified both
enols, C<sub>6</sub>H<sub>9</sub>OH and CH<sub>2</sub>î—»CÂ(OH)–CHî—»CH<sub>2</sub>, and the ionization threshold of C<sub>6</sub>H<sub>9</sub>OH was measured to be 8.2 <i> ± </i> 0.1 eV. Coupled
cluster electronic structure calculations were used to establish the
energetics of MVK. The heats of formation of MVK and its enol were
calculated to be Δ<sub>f</sub><i>H</i><sub>298</sub>(<i>cis</i>-CH<sub>3</sub>CO–CHî—»CH<sub>2</sub>) = −26.1 ± 0.5 kcal mol<sup>–1</sup> and Δ<sub>f</sub><i>H</i><sub>298</sub>(<i>s-cis</i>-1-CH<sub>2</sub>î—»CÂ(OH)–CHî—»CH<sub>2</sub>) = −13.7
± 0.5 kcal mol<sup>–1</sup>. The reaction enthalpy Δ<sub>rxn</sub><i>H</i><sub>298</sub>(C<sub>6</sub>H<sub>10</sub>î—»O → CH<sub>2</sub>î—»CH<sub>2</sub> + <i>s-cis</i>-1-CH<sub>2</sub>î—»CÂ(OH)–CHî—»CH<sub>2</sub>) is 53 ± 1 kcal mol<sup>–1</sup> and Δ<sub>rxn</sub><i>H</i><sub>298</sub>(C<sub>6</sub>H<sub>10</sub>î—»O → CH<sub>2</sub>î—»CH<sub>2</sub> + <i>cis</i>-CH<sub>3</sub>CO–CHî—»CH<sub>2</sub>) is
41 ± 1 kcal mol<sup>–1</sup>. At 1200 K, the products
of cyclohexanone pyrolysis were found to be C<sub>6</sub>H<sub>9</sub>OH, CH<sub>2</sub>î—»CÂ(OH)–CHî—»CH<sub>2</sub>,
MVK, CH<sub>2</sub>CHCH<sub>2</sub>, CO, CH<sub>2</sub>î—»Cî—»O,
CH<sub>3</sub>, CH<sub>2</sub>CCH<sub>2</sub>, CH<sub>2</sub>CH–CHCH<sub>2</sub>, CH<sub>2</sub>CHCH<sub>2</sub>CH<sub>3</sub>, CH<sub>2</sub>CH<sub>2</sub>, and HCCH
Tabletop Femtosecond VUV Photoionization and PEPICO Detection of Microreactor Pyrolysis Products
We
report the combination of tabletop vacuum ultraviolet photoionization
with photoion–photoelectron coincidence spectroscopy for sensitive,
isomer-specific detection of nascent products from a pyrolysis microreactor.
Results on several molecules demonstrate two essential capabilities
that are very straightforward to implement: the ability to differentiate
isomers and the ability to distinguish thermal products from dissociative
ionization. Here, vacuum ultraviolet light is derived from a commercial
tabletop femtosecond laser system, allowing data to be collected at
10 kHz; this high repetition rate is critical for coincidence techniques.
The photoion–photoelectron coincidence spectrometer uses the
momentum of the ion to identify dissociative ionization events and
coincidence techniques to provide a photoelectron spectrum specific
to each mass, which is used to distinguish different isomers. We have
used this spectrometer to detect the pyrolysis products that result
from the thermal cracking of acetaldehyde, cyclohexene, and 2-butanol.
The photoion–photoelectron spectrometer can detect and identify
organic radicals and reactive intermediates that result from pyrolysis.
Direct comparison of laboratory and synchrotron data illustrates the
advantages and potential of this approach
Pyrolysis of the Simplest Carbohydrate, Glycolaldehyde (CHO−CH<sub>2</sub>OH), and Glyoxal in a Heated Microreactor
Both glycolaldehyde and glyoxal were
pyrolyzed in a set of flash-pyrolysis
microreactors. The pyrolysis products resulting from CHO–CH<sub>2</sub>OH and HCO–CHO were detected and identified by vacuum
ultraviolet (VUV) photoionization mass spectrometry. Complementary
product identification was provided by argon matrix infrared absorption
spectroscopy. Pyrolysis pressures in the microreactor were about 100
Torr, and contact times with the microreactors were roughly 100 μs.
At 1200 K, the products of glycolaldehyde pyrolysis are H atoms, CO,
CH<sub>2</sub>O, CH<sub>2</sub>CO, and HCO–CHO.
Thermal decomposition of HCO–CHO was studied with pulsed 118.2
nm photoionization mass spectrometry and matrix infrared absorption.
Under these conditions, glyoxal undergoes pyrolysis to H atoms and
CO. Tunable VUV photoionization mass spectrometry provides a lower
bound for the ionization energy (IE)Â(CHO–CH<sub>2</sub>OH)
≥ 9.95 ± 0.05 eV. The gas-phase heat of formation of glycolaldehyde
was established by a sequence of calorimetric experiments. The experimental
result is Δ<sub>f</sub><i>H</i><sub>298</sub>(CHO–CH<sub>2</sub>OH) = −75.8 ± 1.3 kcal mol<sup>–1</sup>. Fully ab initio, coupled cluster calculations predict Δ<sub>f</sub><i>H</i><sub>0</sub>(CHO–CH<sub>2</sub>OH)
of −73.1 ± 0.5 kcal mol<sup>–1</sup> and Δ<sub>f</sub><i>H</i><sub>298</sub>(CHO–CH<sub>2</sub>OH) of −76.1 ± 0.5 kcal mol<sup>–1</sup>. The
coupled-cluster singles doubles and noniterative triples correction
calculations also lead to a revision of the geometry of CHO–CH<sub>2</sub>OH. We find that the O–H bond length differs substantially
from earlier experimental estimates, due to unusual zero-point contributions
to the moments of inertia
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Thermal Decompositions of the Lignin Model Compounds: Salicylaldehyde and Catechol
The nascent steps
in the pyrolysis of the lignin components salicylaldehyde
(<i>o</i>-HOC<sub>6</sub>H<sub>4</sub>CHO) and catechol
(<i>o</i>-HOC<sub>6</sub>H<sub>4</sub>OH) were studied in
a set of heated microreactors. The microreactors are small (roughly
1 mm ID × 3 cm long); transit times through the reactors are
about 100 μs. Temperatures in the microreactors can be as high
as 1600 K, and pressures are typically a few hundred torr. The products
of pyrolysis are identified by a combination of photoionization mass
spectrometry, photoelectron photoion concidence mass spectroscopy,
and matrix isolation infrared spectroscopy. The main pathway by which
salicylaldehyde decomposes is a concerted fragmentation: <i>o</i>-HOC<sub>6</sub>H<sub>4</sub>CHO (+ M) → H<sub>2</sub> + CO
+ C<sub>5</sub>H<sub>4</sub>î—»Cî—»O (fulveneketene). At
temperatures above 1300 K, fulveneketene loses CO to yield a mixture
of HCî—¼C–ÂCî—¼C–CH<sub>3</sub>, HCî—¼C–ÂCH<sub>2</sub>–Cî—¼CH, and HCî—¼C–ÂCHî—»Cî—»CH<sub>2</sub>. These alkynes decompose to a mixture of radicals (HCî—¼C–ÂCî—¼C–CH<sub>2</sub> and HCî—¼C–CH–ÂCî—¼CH) and H
atoms. H-atom chain reactions convert salicylaldehyde to phenol: <i>o</i>-HOC<sub>6</sub>H<sub>4</sub>CHO + H → C<sub>6</sub>H<sub>5</sub>OH + CO + H. Catechol has similar chemistry to salicylaldehyde.
Electrocyclic fragmentation produces water and fulveneketene: <i>o</i>-HOC<sub>6</sub>H<sub>4</sub>OH (+ M) → H<sub>2</sub>O + C<sub>5</sub>H<sub>4</sub>CO. These findings
have implications for the pyrolysis of lignin itself