33 research outputs found
Oxidative Coupling of Methane: A Microkinetic Model Accounting for Intraparticle Surface-Intermediates Concentration Profiles
A microkinetic model for oxidative
coupling of methane (OCM) has
been developed that comprises a reaction network of 39 gas-phase and
26 catalytic elementary steps. It has been implemented in a heterogeneous
reactor model that explicitly accounts for the interactions between
gas phase and surface species. Concentration gradients arising from
mass transport limitations are found to develop inside the catalyst
pellet for all intermediates (i.e., surface and gas-phase) even under
an intrinsic kinetics regime for the molecules and clearly affect
the C<sub>2</sub> selectivity. Special attention has been devoted
to the reduction of the number of adjustable parameters in the model
and the a priori determination of thermodynamic as well as kinetic
parameters. A contribution analysis is conducted in order to elucidate
the complex reaction pathways in OCM that lead to the desired products.
Apart from the methyl radicals that couple to an extent of almost
70% in the void space between the pellets, the catalyst pellet accounts
for the majority of molecules and radicals conversion, which are produced
on the surface and further interact either in the catalyst pores or
with other surface species. Almost 95% of CH<sub>4</sub> consumption
and more than half of the C<sub>2</sub>H<sub>6</sub> production take
place inside the catalyst pellet. A similar analysis is applied to
understand the effect of various textural properties of catalysts
on the performance of OCM, for example, increasing the catalyst porosity
is found beneficial for the C<sub>2</sub> yield, as long as a sufficient
CH<sub>4</sub> activation takes place, so that the coupling pathway
is promoted over the heterogeneous oxidation of CH<sub>3</sub><b>Ā·</b>
DFT Investigation into Alumina ALD Growth Inhibition on Hydroxylated Amorphous Silica Surface
Alumina
(Al<sub>2</sub>O<sub>3</sub>), a suitable replacement for
silica (SiO<sub>2</sub>) as gate oxide in metal oxide semiconductor
field effect transistors (MOSFET), is deposited on the amorphous silica
layer of the semiconductor substrate by atomic layer deposition (ALD)
using trimethylaluminum (TMA) and water as precursors. A computationally
efficient model for the hydroxylated amorphous silica surface is obtained
by means of molecular dynamics and is used to investigate the reason
behind the observed growth inhibition during alumina ALD. The reactions
of TMA are investigated by periodic DFT calculations on surfaces with
hydroxyl coverage of 3.38 OH nm<sup>ā2</sup> and 5.07 OH nm<sup>ā2</sup>. The formation of SiCH<sub>3</sub> surface species
is found to be possible only on the less hydroxylated surface during
the first TMA half-cycle, while the subsequent reaction of water with
the SiCH<sub>3</sub> surface species is found to be highly activated
(<i>E</i><sub>a</sub> = 196 kJ mol<sup>ā1</sup>).
Since these SiCH<sub>3</sub> surface species are rather unreactive
toward water, fewer hydroxyls are regenerated during this first water
half-cycle, resulting in the observed initial growth inhibition. Moreover,
alumina growth can continue over the aluminum surface species, trapping
the unreactive SiCH<sub>3</sub> species at the interface between deposited
alumina and silica. Such carbon impurities at the interface should
be avoided nonetheless, since they can create undesirable tunneling
currents in MOSFETs
Assessment of a GasāSolid Vortex Reactor for SO<sub>2</sub>/NO<sub><i>x</i></sub> Adsorption from Flue Gas
The feasibility of performing the SO<sub>2</sub>/NO<sub><i>x</i></sub> adsorption process in a gasāsolid
vortex
reactor (GSVR) is examined and compared with the more traditional
riser technology. The multiphase reacting flow is modeled using the
EulerianāEulerian two-fluid model. Models of nonreacting flows
were validated using data from a bench-scale experimental setup. The
GSVR has the potential to significantly improved heat/mass transfer
between phases, as compared to more conventional fluidization technologies.
Process intensification opportunities are investigated. The model
predicts continuous removal efficiencies greater than 99% for SO<sub>2</sub> and approximately 80% for NO<sub><i>x</i></sub>. The gasāsolid slip velocity and convective mass transfer
coefficient for the riser were 0.2ā0.5 and 0.06ā0.12
m/s, respectively, whereas the values for the GSVR were 6ā7
and 1.0ā1.1 m/s, respectively. This order of magnitude increase
in the external mass transfer coefficient highlights the potential
intensification opportunities provided by the GSVR
Combined Comprehensive Two-Dimensional Gas Chromatography Analysis of Polyaromatic Hydrocarbons/Polyaromatic Sulfur-Containing Hydrocarbons (PAH/PASH) in Complex Matrices
A new
gas chromatographic method has been developed that is able
to quantify polycyclic aromatic hydrocarbons (PAH) and polycyclic
aromatic sulfur-containing hydrocarbons (PASH) up to four rings. The
method combines the power of both flame ionization detection (FID)
and sulfur chemiluminescence detection (SCD) in series on a single
comprehensive two-dimensional gas chromatography (GC Ć GC) system
and provides mass fractions of compounds separated by carbon number <i>n</i> (C<sub><i>n</i></sub>H<sub><i>x</i></sub>S<sub><i>y</i></sub>) and class. In addition to PAH
and PASH separation, the method is extended toward nonaromatic and
monoaromatic (sulfur-containing) compounds (paraffins, naphthenes,
monoaromatics, thiols, sulfides, disulfides, and thiophenes). The
95% confidence interval is doubled when a single injection technique
is used instead of a more-accurate double injection technique. A flexible
correction procedure that combines the advantages of the two-dimensional
separation of GC Ć GC and its ability to easily define overlapping
groups between the FID and the SCD chromatograms is applied. The method
is validated using theoretical reference mixtures and is applied on
three commercial gas oils with sulfur content from 0.16 wtā%
up to 1.34 wtā%. The repeatability is good, with an average
of 3.4%, which is in the same range as the much more expensive Fourier
transform ion cyclotron resonanceāmass spectroscopy (FTICR-MS)
technique
Isobutene Protonation in HāFAU, HāMOR, HāZSM-5, and HāZSM-22
Kinetics and thermodynamics of isobutene protonation
in H-FAU,
H-MOR, H-ZSM-5, and H-ZSM-22 have been studied in a temperature range
of 300ā800 K, combining PW91-D//PW91 periodic density functional
theory calculations with statistical thermodynamics. At temperatures
relevant for industrial zeolite-catalyzed processes (500ā800
K), the <i>tert</i>-butyl carbenium ion is more stable than
the <i>tert</i>-butoxy in H-MOR, H-ZSM-5, and H-ZSM-22.
Entropy contributions govern the standard Gibbs free energy stability
of the chemisorbed intermediates. Due to the absence of a CāO
covalent bond, formation of the <i>tert</i>-butyl carbenium
ion is accompanied by a lower entropy loss and, consequently, has
a higher stability than the <i>tert</i>-butoxy in H-MOR,
H-ZSM-5, and H-ZSM-22. At 800 K, the protonation toward <i>tert</i>-butoxy in H-FAU, H-MOR, and H-ZSM-5 and to the <i>tert</i>-butyl carbenium ion in H-ZSM-22 is 5 to 7 orders of magnitude faster
than the protonation toward isobutoxy. Among the four zeolites, the
lowest activation energy is found in H-ZSM-22
Coking Resistance of Specialized Coil Materials during Steam Cracking of Sulfur-Free Naphtha
The reactor material strongly affects
coke formation during steam
cracking of hydrocarbons. Therefore, in the past decade several specialized
reactor materials have been developed that have proven to be efficient
in reducing coke formation for ethane steam cracking. However, their
beneficial anticoking properties are questioned when heavier feedstocks
such as naphtha are cracked. Therefore, the effect of the composition
of the reactor material has been investigated for ethane and naphtha
cracking in an electrobalance setup under industrially relevant conditions.
A significant reduction of coke formation is obtained for specialized
alloys compared to typical FeāCrāNi heat resistant steels
when a sulfur-free naphtha is cracked. A thin layer of alumina on
the surface along with manganese chromite provides the highest resistance
to coking, as was demonstrated by the SEM and EDX analyses. The decrease
in coking rate translates in a run length increase of 50% for a typical
naphtha furnace equipped with reactors made out of an Al-enhanced
alloy instead of typically applied heat resistant steel
Influence of the Reactor Material Composition on Coke Formation during Ethane Steam Cracking
An
experimental study of the coking tendency of nine different
materials was carried out in a quartz electrobalance setup with a
jet stirred reactor (JSR) under industrially relevant ethane steam
cracking conditions: <i>T</i><sub>material</sub> = 1159
K, <i>P</i><sub>tot</sub> = 0.1 MPa, Ļ<sub>ethane</sub> = 73%, dilution Ī“ = 0.33 kg<sub>H2O</sub>/kg<sub>HC</sub>.
A strong influence of the composition of the materials on the coking
rate as a function of time on-stream was observed. The initial coking
rate varied from 5 Ć 10<sup>ā4</sup> gĀ·m<sup>ā2</sup>Ā·s<sup>ā1</sup> to 27 Ć 10<sup>ā4</sup> gĀ·m<sup>ā2</sup>Ā·s<sup>ā1</sup>, while the asymptotic
coking rate changed in the range of 2 Ć 10<sup>ā4</sup> gĀ·m<sup>ā2</sup>Ā·s<sup>ā1</sup> to 6 Ć
10<sup>ā4</sup> gĀ·m<sup>ā2</sup>Ā·s<sup>ā1</sup>. SEM and EDX analyses of coked and uncoked coupons revealed that
the composition of the oxide layer in contact with the cracked gas,
formed after the initial preoxidation or decoking, has an important
influence on the amount of coke deposited. Materials that formed a
thin Al<sub>2</sub>O<sub>3</sub> layer on the coupon surface showed
a higher coking resistance. A uniform surface composition and a high
resistance to spalling and fractures are other important characteristics
of good materials
Advanced Elemental Characterization during PtāIn Catalyst Formation by Wavelet Transformed Xāray Absorption Spectroscopy
Complementary to conventional X-ray
absorption near edge structure
(XANES) and Fourier transformed (FT) extended X-ray absorption fine
structure (EXAFS) analysis, the systematic application of wavelet
transformed (WT) XAS is shown to disclose the physicochemical mechanisms
governing PtāIn catalyst formation. The simultaneous k- and
R-space resolution of the WT XAS signal allows for the efficient allocation
of the elemental nature to each R-space peak. Because of its elemental
discrimination capacity, the technique delivers structural models
which can subsequently serve as an input for quantitative FT EXAFS
modeling. The advantages and limitations of applying WT XAS are demonstrated
(1) before and (2) after calcination to 650 Ā°C of a PtĀ(acac)<sub>2</sub> impregnated MgĀ(In)Ā(Al)ĀO<sub><i>x</i></sub> support
and (3) after subsequent H<sub>2</sub> reduction to 650 Ā°C. Combined
XANES, FT, and WT XAS analysis shows that the acac ligands of the
Pt precursor decompose during calcination, leading to atomically dispersed
Pt<sup>4+</sup> cations on the MgĀ(In)Ā(Al)ĀO<sub><i>x</i></sub> support. H<sub>2</sub> reduction treatment eventually results in
the formation of 1.5 nm PtāIn alloyed nanoparticles. Widespread
use and systematic application of wavelet-based XAS can potentially
reveal in greater detail the intricate mechanisms involved in catalysis,
chemistry, and related fields
Coking Tendency of 25Cr-35Ni Alloys: Influence of Temperature, Sulfur Addition, and Cyclic Aging
25Cr-35Ni
base alloys are the most frequently used materials for
steam cracking reactors. The influence of cyclic aging, reactor temperature,
and adding sulfur containing compounds before or during cracking on
the rate of coke deposition on a classical 25Cr-35Ni alloy is evaluated
using a jet stirred reactor equipped with an electrobalance. As expected,
the initial and asymptotic coking rate increased with increasing reactor
temperature. Scanning electron microscopy coupled with energy dispersive
X-ray (SEM-EDX) analysis indicated that more Ni and Fe is present
on the surface at higher cracking temperatures. Presulfidation led
to increased coke deposition and decreased CO yields compared to the
reference. When a sulfur containing compound was added continuously,
coke deposition increased significantly but carbon oxide formation
was suppressed. A pronounced amount of coke was measured in the reactor,
followed by suppressed generated amounts of carbon oxides downstream.
When combined with the continuous addition of sulfur containing compounds,
presulfidation has little effect. Depending on the conditions, the
effect of aging of the material is different: during the reference
run and when only presulfidation was applied, coking rates increased
as the material aged. When sulfur containing compounds were added
continuously, with our without presulfidation, coking rates decreased
as the material aged. This can be related with increased amounts of
MnCr<sub>2</sub>O<sub>4</sub> and Cr<sub>2</sub>O<sub>3</sub> observed
by SEM and EDX analysis
Periodic DFT Study of Benzene Adsorption on Pd(100) and Pd(110) at Medium and Saturation Coverage
Benzene
adsorption on Pd(100) and Pd(110) has been investigated using periodic
density functional theory (DFT) calculations. 4-Fold hollow geometries
are preferentially adopted on both surfaces, and due to stronger repulsive
interactions on Pd(100) a larger decrease in adsorption energy is
calculated from medium to saturation coverage (ā¼120 kJ mol<sup>ā1</sup>) compared to Pd(110) (ā¼15 kJ mol<sup>ā1</sup>). On Pd(100), a slight energetic preference is calculated at saturation
coverage for an adsorbate with two CC bonds parallel to the [011Ģ
]
direction. However, an adsorption geometry with alternately two types
of benzene adsorbates, rotated azimuthally by 30Ā° relative to
one another, cannot be discarded since both geometries are compatible
with ultraviolet photoemission spectroscopy (UPS) and high-resolution
electron energy loss spectroscopy (HREELS) observations. On Pd(110),
there is a slight energetic preference for the hollow(0) site relative
to the hollow(15) and hollow(30) at saturation coverage, and their
calculated electronic features match UPS experiments. For the hollow(30),
calculated vibrational features are not compatible with HREELS experiments,
indicating that benzene does not populate hollow(30) sites at saturation
coverage. Calculated STM images confirm that the experimentally observed
two-lobed protrusion separated by a single depression oriented with
its direction some 50Ā° from [11Ģ
0] can only correspond
to the hollow(15) adsorbate. Inclusion of van der Waals interactions
(vdW-DFT) increases adsorption energies by some 50 kJ mol<sup>ā1</sup>, but the relative ordering of the various adsorption sites remains
unaltered as compared to PW91