7 research outputs found
Experimental and Theoretical Studies into the Formation of C<sub>4</sub>–C<sub>6</sub> Products in Partially Chlorinated Hydrocarbon Pyrolysis Systems: A Probabilistic Approach to Congener-Specific Yield Predictions
This work presents a study of the
pyrolytic formation of vinylacetylene
and benzene congeners formed from chlorinated hydrocarbon precursors,
a complex, multipath polymerization system formed in a monomer-rich
environment. (Co-)Âpyrolyses of dichloro- and trichloroethylene yield
a rich array of products, and assuming a single dominant underlying
growth mechanism, this (on comparing expected and observed products)
allows a number of potentially competing channels to C<sub>4</sub> and C<sub>6</sub> products to be ruled out. Poor congener/isomer
descriptions rule out even-carbon radical routes, and the absence
of C<sub>3</sub> and C<sub>5</sub> products rule out odd-carbon processes.
Vinylidenes appear unable to describe the increased reactivity of
acetylenes with chlorination noted in our experiments, leaving molecular
acetylene dimerization processes and, in C<sub>6</sub> systems, the
closely related Diels–Alder cyclization as the likely reaction
mechanism. The feasibility of these routes is further supported by
ab initio calculations. However, some of the most persuasive evidence
is provided by congener-specific yield predictions enabled by the
construction of a probability tree analogue of kinetic modeling. This
approach is relatively quick to construct, provides surprisingly accurate
predictions, and may be a very useful tool in screening for important
reaction channels in poorly understood congener- or isomer-rich reaction
systems
Molecular Mechanisms in the Pyrolysis of Unsaturated Chlorinated Hydrocarbons: Formation of Benzene Rings. 1. Quantum Chemical Studies
Analogues of important aromatic growth
mechanisms in hydrocarbon pyrolysis and combustion systems are extended
to chlorinated systems. We consider the addition of C<sub>2</sub>Cl<sub>2</sub> to both C<sub>4</sub>Cl<sub>3</sub> and C<sub>4</sub>Cl<sub>5</sub> radicals at the M06-2X/6-311+GÂ(3df,3p)//B3LYP/6-31GÂ(d) level
of theory, and we demonstrate that these reaction systems have much
in common with those of nonchlorinated species. In particular, we
find that these radicals appear to lead preferentially to fulvenes,
and not to the observed aromatic products, as is found in nonchlorinated
systems. We have therefore also considered nonradical C<sub>4</sub>/C<sub>2</sub> channels by way of Diels–Alder cyclization
of C<sub>4</sub>Cl<sub>4</sub>/C<sub>2</sub>Cl<sub>2</sub> and C<sub>4</sub>H<sub>2</sub>Cl<sub>2</sub>/C<sub>2</sub>HCl pairs to describe
aromatic formation. While the latter pair readily leads to the formation
of partially chlorinated benzenes, the fully chlorinated congeners
are sterically prohibited from ring closing directly; this leads to
a series of novel rearrangement processes which predict the formation
of hexachloro-1,5-diene-3-yne, in addition to hexachlorobenzene, in
good agreement with experiment. This suggests, for the first time,
that facile nonradical routes to aromatic formation are operative
in partially and fully chlorinated pyrolysis and combustion systems
High Temperature Chemistry of Chlorinated Acenaphthylene. 3C Bay Acetylene Additions and Annealing by Five-Membered Ring Shifts
Experimental and theoretical results
concerning the growth and
isomerization of chlorinated acenaphthylene, C<sub>12</sub>H<sub>8</sub>, during the pyrolysis of chlorohydrocarbons are presented here.
A fullerene subunit, C<sub>12</sub>H<sub>8</sub>, is a useful system
to investigate regarding C<sub>60</sub> formation. However, direct
experimental observation of isomerization and annealing processes
in particular are difficult to confirm due to the high symmetry of
the parent molecule. Chlorination lowers the symmetry, essentially
labeling carbon atoms, allowing growth and isomerization to be followed
directly. Pyrolysis of dichloro- and trichloroethylene, and their
copyrolyses with trichlorobenzenes, provides an efficient and general
source of chlorinated acenaphthylenes in a range of degrees of chlorination
and over a number of unique congeners. Analysis of congener yields
as a function of reagents employed, guided by DFT/B3LYP/6-311GÂ(d,p)
level calculations, strongly suggests that C<sub>2</sub> addition
across three-carbon bays in naphthalene is a major driver of growth.
Additionally, extremely facile five-membered ring shifts are operative,
with chlorine promoting isomerization. Theoretical study of C<sub>16</sub>H<sub>10</sub>- and C<sub>18</sub>H<sub>10</sub>-based congeners
indicate that this is a general phenomenon, and with chlorine also
favoring internal cyclopentafused rings in addition to increased isomerization
rates, this suggests halogen moieties may be an important feature
for efficient fullerene growth
Role of Hydrogen Abstraction Acetylene Addition Mechanisms in the Formation of Chlorinated Naphthalenes. 2. Kinetic Modeling and the Detailed Mechanism of Ring Closure
The dominant formation mechanisms
of chlorinated phenylacetylenes,
naphthalenes, and phenylvinylacetylenes in relatively low pressure
and temperature (∼40 Torr and 1000 K) pyrolysis systems are
explored. Mechanism elucidation is achieved through a combination
of theoretical and experimental techniques, the former employing a
novel simplification of kinetic modeling which utilizes rate constants
in a probabilistic framework. Contemporary formation schemes of the
compounds of interest generally require successive additions of acetylene
to phenyl radicals. As such, infrared laser powered homogeneous pyrolyses
of dichloro- or trichloroethylene were perturbed with 1,2,4- or 1,2,3-trichlorobenzene.
The resulting changes in product identities were compared with the
major products expected from conventional pathways, aided by the results
of our previous computational work. This analysis suggests that a
Bittner–Howard growth mechanism, with a novel amendment to
the conventional scheme made just prior to ring closure, describes
the major products well. Expected products from a number of other
potentially operative channels are shown to be incongruent with experiment,
further supporting the role of Bittner–Howard channels as the
unique pathway to naphthalene growth. A simple quantitative analysis
which performs very well is achieved by considering the reaction scheme
as a probability tree, with relative rate constants being cast as
branching probabilities. This analysis describes all chlorinated phenylacetylene,
naphthalene, and phenylvinylacetylene congeners. The scheme is then
tested in a more general system, i.e., not enforcing a hydrogen abstraction/acetylene
addition mechanism, by pyrolyzing mixtures of di- and trichloroethylene
without the addition of an aromatic precursor. The model indicates
that these mechanisms are still likely to be operative
Adsorptive Capacity and Evolution of the Pore Structure of Alumina on Reaction with Gaseous Hydrogen Fluoride
Brunauer–Emmet–Teller
(BET) specific surface areas
are generally used to gauge the propensity of uptake on adsorbents,
with less attention paid to kinetic considerations. We explore the
importance of such parameters by modeling the pore size distributions
of smelter grade aluminas following HF adsorption, an industrially
important process in gas cleaning at aluminum smelters. The pore size
distributions of industrially fluorinated aluminas, and those contacted
with HF in controlled laboratory trials, are reconstructed from the
pore structure of the untreated materials when filtered through different
models of adsorption. These studies demonstrate the presence of three
distinct families of pores: those with uninhibited HF uptake, kinetically
limited porosity, and pores that are surface blocked after negligible
scrubbing. The surface areas of the inaccessible and blocked pores
will overinflate estimates of the adsorption capacity of the adsorbate.
We also demonstrate, contrary to conventional understanding, that
porosity changes are attributed not to monolayer uptake but more reasonably
to pore length attenuation. The model assumes nothing specific regarding
the Al<sub>2</sub>O<sub>3</sub>–HF system and is therefore
likely general to adsorbate/adsorbent phenomena
The Influence of Surface Structure on H<sub>4</sub>SiO<sub>4</sub> Oligomerization on Rutile and Amorphous TiO<sub>2</sub> Surfaces: An ATR-IR and Synchrotron XPS Study
Silicic acid (H<sub>4</sub>SiO<sub>4</sub>) is ubiquitous
in natural
aquatic systems. Applications of TiO<sub>2</sub> in these systems
will be influenced by H<sub>4</sub>SiO<sub>4</sub> sorption and oligomerization
reactions on the TiO<sub>2</sub> surface, and this can affect many
aspects of TiO<sub>2</sub> reactivity. The spatial arrangement of
sorption sites on a metal oxide surface can promote specific lateral
interactions, such as oligomerization, between sorbed species. In
this work we explore the relationship between surface structure and
interfacial H<sub>4</sub>SiO<sub>4</sub> oligomerization by quantifying
the extent of H<sub>4</sub>SiO<sub>4</sub> sorption and oligomerization
on three TiO<sub>2</sub> phases; a rutile phase having well-developed
(110) faces (R180), a rutile phase with poorly developed (110) faces
(R60), and an amorphous TiO<sub>2</sub> (TiO<sub>2(am)</sub>). The <i>in situ</i> ATR-IR spectra measured over time as 0.2 mM H<sub>4</sub>SiO<sub>4</sub> reacted with TiO<sub>2</sub> were quite different
on the three TiO<sub>2</sub> phases. The percentage of the surface
H<sub>4</sub>SiO<sub>4</sub> that was present as oligomers increased
over time on all phases, but after 20 h almost all H<sub>4</sub>SiO<sub>4</sub> on the R180 surface was oligomeric, while the H<sub>4</sub>SiO<sub>4</sub> on TiO<sub>2(am)</sub> was predominantly monomeric.
The extent of H<sub>4</sub>SiO<sub>4</sub> oligomerization on R60
was intermediate. When the TiO<sub>2</sub> phases reacted with 1.5
mM H<sub>4</sub>SiO<sub>4</sub> the ATR-IR spectra showed oligomeric
silicates dominating the surface of all three TiO<sub>2</sub> phases;
however, after 20 h the percentage of the surface H<sub>4</sub>SiO<sub>4</sub> present as three-dimensional polymers was ∼30, 10,
and 0% on R180, R60, and TiO<sub>2(am)</sub> respectively. The Si
2s photoelectron peak binding energy (BE) and the H<sub>4</sub>SiO<sub>4</sub> surface coverage (Γ<sub>Si</sub>) were measured by
XPS over a range of Γ<sub>Si</sub>. For any given Γ<sub>Si</sub> the Si 2s BE’s were in the order R180 > R60 >
TiO<sub>2(am)</sub>. A higher Si 2s BE indicates a greater degree
of silicate
polymerization. The ATR-IR and XPS results support the existing model
for interfacial H<sub>4</sub>SiO<sub>4</sub> oligomerization where
linear trimeric silicates are formed by insertion of a solution H<sub>4</sub>SiO<sub>4</sub> between suitably orientated adjacent bidentate
sorbed monomers. The TiO<sub>2(am)</sub> has previously been shown
to consist of ∼2 nm diameter particles with a highly disordered
surface. When compared to the TiO<sub>2(am)</sub> surface, the regular
arrangement of TiO<sub>6</sub> octahedra on the rutile (110) face
means that sorbed H<sub>4</sub>SiO<sub>4</sub> monomers on adjacent
rows of singly coordinated oxygen atoms are oriented so as to favor
linear trimer formation. Higher silicate polymers can form between
adjacent trimers, and this is favored on the rutile (110) surfaces
compared to the TiO<sub>2(am)</sub>. This is also expected on the
basis of the arrangement of surface sites on the rutile (110) surface
and because the high surface curvature inherent in a ∼2 nm
spherical TiO<sub>2(am)</sub> particle would increase the spatial
separation of adjacent trimers
The Influence of Surface Structure on H<sub>4</sub>SiO<sub>4</sub> Oligomerization on Rutile and Amorphous TiO<sub>2</sub> Surfaces: An ATR-IR and Synchrotron XPS Study
Silicic acid (H<sub>4</sub>SiO<sub>4</sub>) is ubiquitous
in natural
aquatic systems. Applications of TiO<sub>2</sub> in these systems
will be influenced by H<sub>4</sub>SiO<sub>4</sub> sorption and oligomerization
reactions on the TiO<sub>2</sub> surface, and this can affect many
aspects of TiO<sub>2</sub> reactivity. The spatial arrangement of
sorption sites on a metal oxide surface can promote specific lateral
interactions, such as oligomerization, between sorbed species. In
this work we explore the relationship between surface structure and
interfacial H<sub>4</sub>SiO<sub>4</sub> oligomerization by quantifying
the extent of H<sub>4</sub>SiO<sub>4</sub> sorption and oligomerization
on three TiO<sub>2</sub> phases; a rutile phase having well-developed
(110) faces (R180), a rutile phase with poorly developed (110) faces
(R60), and an amorphous TiO<sub>2</sub> (TiO<sub>2(am)</sub>). The <i>in situ</i> ATR-IR spectra measured over time as 0.2 mM H<sub>4</sub>SiO<sub>4</sub> reacted with TiO<sub>2</sub> were quite different
on the three TiO<sub>2</sub> phases. The percentage of the surface
H<sub>4</sub>SiO<sub>4</sub> that was present as oligomers increased
over time on all phases, but after 20 h almost all H<sub>4</sub>SiO<sub>4</sub> on the R180 surface was oligomeric, while the H<sub>4</sub>SiO<sub>4</sub> on TiO<sub>2(am)</sub> was predominantly monomeric.
The extent of H<sub>4</sub>SiO<sub>4</sub> oligomerization on R60
was intermediate. When the TiO<sub>2</sub> phases reacted with 1.5
mM H<sub>4</sub>SiO<sub>4</sub> the ATR-IR spectra showed oligomeric
silicates dominating the surface of all three TiO<sub>2</sub> phases;
however, after 20 h the percentage of the surface H<sub>4</sub>SiO<sub>4</sub> present as three-dimensional polymers was ∼30, 10,
and 0% on R180, R60, and TiO<sub>2(am)</sub> respectively. The Si
2s photoelectron peak binding energy (BE) and the H<sub>4</sub>SiO<sub>4</sub> surface coverage (Γ<sub>Si</sub>) were measured by
XPS over a range of Γ<sub>Si</sub>. For any given Γ<sub>Si</sub> the Si 2s BE’s were in the order R180 > R60 >
TiO<sub>2(am)</sub>. A higher Si 2s BE indicates a greater degree
of silicate
polymerization. The ATR-IR and XPS results support the existing model
for interfacial H<sub>4</sub>SiO<sub>4</sub> oligomerization where
linear trimeric silicates are formed by insertion of a solution H<sub>4</sub>SiO<sub>4</sub> between suitably orientated adjacent bidentate
sorbed monomers. The TiO<sub>2(am)</sub> has previously been shown
to consist of ∼2 nm diameter particles with a highly disordered
surface. When compared to the TiO<sub>2(am)</sub> surface, the regular
arrangement of TiO<sub>6</sub> octahedra on the rutile (110) face
means that sorbed H<sub>4</sub>SiO<sub>4</sub> monomers on adjacent
rows of singly coordinated oxygen atoms are oriented so as to favor
linear trimer formation. Higher silicate polymers can form between
adjacent trimers, and this is favored on the rutile (110) surfaces
compared to the TiO<sub>2(am)</sub>. This is also expected on the
basis of the arrangement of surface sites on the rutile (110) surface
and because the high surface curvature inherent in a ∼2 nm
spherical TiO<sub>2(am)</sub> particle would increase the spatial
separation of adjacent trimers