15 research outputs found
Large-Grain, Oriented, and Thin Zeolite MFI Films from Directly Synthesized Nanosheet Coatings
Directly
synthesized zeolite MFI nanosheets are promising building
blocks for MFI thin films with large and oriented grains. The secondary
growth of MFI nanosheets on Si wafers in tetraethylammonium hydroxide
(TEAOH) silica sols was investigated, and conditions that result in
well-oriented and intergrown film microstructure were established.
This has enabled the fabrication of thin (∼300 nm) <i>b</i>-oriented MFI films with large grain-size (>2 μm)
from seed-removed nanosheet monolayer coatings. Moreover, the faceted
and anisotropic shape of MFI nanosheets allowed the measurement of
MFI growth in different crystallographic directions and confirmed
the twinning-free preferential growth along the <i>c</i>-axis (a lateral direction of the nanosheet), compared to the <i>b</i>-axis (the direction normal to the nanosheet basal plane),
with ratios in a range between 4 and 11
TraPPE-zeo: Transferable Potentials for Phase Equilibria Force Field for All-Silica Zeolites
The transferable potentials for phase
equilibria (TraPPE) force
field is extended to all-silica zeolites. This novel force field is
parametrized to match the experimental adsorption isotherms of <i>n</i>-heptane, propane, carbon dioxide, and ethanol with the
Lennard-Jones parameters for sorbate–framework interactions
determined in a consistent manner using the Lorentz–Berthelot
combining rules as for other parts of the TraPPE force field. The
TraPPE-zeo force field allows for accurate predictions for both adsorption
and diffusion of alkanes, alcohols, carbon dioxide, and water over
a wide range of pressures and temperatures. In order to achieve transferability
to a wider range of molecule types, ranging from nonpolar to dipolar
and hydrogen-bonding compounds, Lennard-Jones interaction sites and
partial charges are placed at both the oxygen and the silicon atoms
of the zeolite lattice, which allows for a better balance of dispersive
and first-order electrostatic interactions than is achievable with
the Lennard-Jones potential used only for the oxygen atoms. The use
of the Lorentz–Berthelot combining rules for unlike interactions
makes the TraPPE-zeo force field applicable to any sorbate as long
as the relevant TraPPE sorbate–sorbate parameters are available.
The TraPPE-zeo force field allows for greatly improved predictive
power compared to force fields that explicitly tabulate the individual
cross-interaction parameters
One-Pot Synthesis of 5-(Ethoxymethyl)furfural from Glucose Using Sn-BEA and Amberlyst Catalysts
5-(Ethoxymethyl)Âfurfural (EMF) was produced from glucose
in ethanol
in a single reactor at 90 °C. The reaction proceeds via the isomerization
of glucose to fructose with zeolite Sn-Beta, a Lewis acid catalyst.
Fructose is converted to 5-(hydroxymethyl)Âfurfural, which is then
etherified to EMF using a Brønsted acid catalyst, Amberlyst 131.
An EMF yield of 31% was achieved
Development of the Transferable Potentials for Phase Equilibria Model for Hydrogen Sulfide
The transferable potentials for phase
equilibria force field is
extended to hydrogen sulfide. The pure-component and binary vapor–liquid
equilibria with methane and carbon dioxide and the liquid-phase relative
permittivity are used for the parametrization of the Lennard–Jones
(LJ) and Coulomb interactions, and models with three and four interaction
sites are considered. For the three-site models, partial point charges
are placed on the sites representing the three atoms, while the negative
partial charge is moved to an off-atom site for the four-site models.
The effect of molecular shape is probed using either only a single
LJ interaction site on the sulfur atom or adding sites also on the
hydrogen atoms. This procedure results in four distinct models, but
only those with three LJ sites can accurately reproduce all properties
considered for the parametrization. These two are further assessed
for predictions of the liquid-phase structure, the lattice parameters
and relative permittivity for the face-centered-cubic solid, and the
triple point. An effective balance between LJ interactions and the
dipolar and quadrupolar terms of the first-order electrostatic interactions
is struck in order to obtain a four-site model that describes the
condensed-phase properties and the phase equilibria with high accuracy
Combining Pre- and Post-Nucleation Trajectories for the Synthesis of High FAU-Content Faujasite Nanocrystals from Organic-Free Sols
The
effects of synthesis conditions on the FAU/EMT content and
the size of nanocrystals, formed from inorganic aluminosilicate sols,
were investigated. High-resolution transmission electron microscopy
imaging and comparison of experimental X-ray diffraction patterns
with simulations demonstrated that all materials made starting from
synthesis mixtures in the composition range (1.8–33) SiO<sub>2</sub>:1 Al<sub>2</sub>O<sub>3</sub>:(2.7–33) Na<sub>2</sub>O:(41–1000) H<sub>2</sub>O contain FAU/EMT intergrowths. Compositions
with low water content increase the FAU fraction up to 0.8 but the
crystal size exceeds 100 nm. Extension of the higher FAU purity to
nanocrystals was achieved only by first mixing the sol at high water
content compositions that favor nanocrystal formation and thenî—¸after
a certain timeî—¸lowering by freeze-drying the water to levels
favoring the formation of FAU. Cryogenic transmission electron microscopy
and small-angle X-ray scattering from representative optically clear
and colloidally stable precursor sols (aged and crystallized at ambient
temperature) reveal the formation of amorphous aggregates before the
detection of crystals, in agreement with earlier findings and an existing
model for the aggregative growth of the zeolite MFI. The presence
of these amorphous aggregates coincides with the aforementioned state
of sol that preserves the original trajectory toward nanocrystals
after the pronounced reduction of water content by freeze-drying.
If water reduction by freeze-drying is applied earlier (before the
detection of amorphous aggregates), the sol follows the low water
content trajectory toward larger crystals. Despite this memory effect,
the sol at this stage is still agnostic toward FAU or EMT formation,
the relative content of which is dominantly determined by the final
water content. These findings demonstrate that it is possible to combine
the effects of pre- and post-nucleation sol composition to steer crystal
size and crystal structure, respectively. They confirm precursor nanoparticle
evolution, while they emphasize the importance of solution phase composition
at both pre- and post-nucleation stages of aggregative crystal growth
Direct Synthesis of 7 nm-Thick Zinc(II)–Benzimidazole–Acetate Metal–Organic Framework Nanosheets
Direct Synthesis
of 7 nm-Thick Zinc(II)–Benzimidazole–Acetate
Metal–Organic Framework Nanosheet
Understanding Diffusion in Hierarchical Zeolites with House-of-Cards Nanosheets
Introducing
mesoporosity to conventional microporous sorbents or
catalysts is often proposed as a solution to enhance their mass transport
rates. Here, we show that diffusion in these hierarchical materials
is more complex and exhibits non-monotonic dependence on sorbate loading.
Our atomistic simulations of <i>n</i>-hexane in a model
system containing microporous nanosheets and mesopore channels indicate
that diffusivity can be smaller than in a conventional zeolite with
the same micropore structure, and this observation holds true even
if we confine the analysis to molecules completely inside the microporous
nanosheets. Only at high sorbate loadings or elevated temperatures,
when the mesopores begin to be sufficiently populated, does the overall
diffusion in the hierarchical material exceed that in conventional
microporous zeolites. Our model system is free of structural defects,
such as pore blocking or surface disorder, that are typically invoked
to explain slower-than-expected diffusion phenomena in experimental
measurements. Examination of free energy profiles and visualization
of molecular diffusion pathways demonstrates that the large free energy
cost (mostly enthalpic in origin) for escaping from the microporous
region into the mesopores leads to more tortuous diffusion paths and
causes this unusual transport behavior in hierarchical nanoporous
materials. This knowledge allows us to re-examine zero-length-column
chromatography data and show that these experimental measurements
are consistent with the simulation data when the crystallite size
instead of the nanosheet thickness is used for the nominal diffusional
length
Density Functional Theory Study on the Adsorption of H<sub>2</sub>S and Other Claus Process Tail Gas Components on Copper- and Silver-Exchanged Y Zeolites
The potential use of Cu- and Ag-exchanged Y zeolites as selective adsorbents for hydrogen sulfide (H<sub>2</sub>S) from Claus process tail gas was investigated with density functional theory (DFT). The adsorption energies of H<sub>2</sub>S and other Claus tail gas components (CO, H<sub>2</sub>O, N<sub>2</sub>, and CO<sub>2</sub>) were computed for these zeolites as well as for Li–Y, Na–Y, and K–Y on a cluster model. Comparison of adsorption energies for H<sub>2</sub>S versus the other components indicated that Ag–Y has potential for selective adsorption of H<sub>2</sub>S, whereas Cu–Y is subject to strong adsorption of CO, and alkali metal-exchanged Y zeolites are subject to H<sub>2</sub>O adsorption. Comparison with alkali metal-exchanged Y zeolites was performed to clarify the role of d electrons, while the influence of the zeolite framework was assessed by comparing adsorption energies on the cluster model with those on bare cations. Absolutely localized molecular orbital energy decomposition analysis (ALMO EDA) revealed that for Cu- and Ag-containing systems, transfer of electrons between the cation and the adsorbate, i.e., the donation of d electrons and the acceptance of electrons in the unoccupied orbitals of the cation, plays an important role in determining the adsorption energy. On the other hand, for alkali metals-containing systems, charge transfer is negligible and adsorption energies are dominated by interactions due to electrostatics, polarization, and structural distortions
Probing the Relationship between Silicalite‑1 Defects and Polyol Adsorption Properties
The relationship between polyol adsorption
affinity and silanol defect density was investigated through the development
of vapor and aqueous adsorption isotherms on silicalite-1 materials
which vary in structural and surface properties. Silicalite-1 crystals
prepared through alkaline synthesis, alkaline synthesis with steaming
post-treatment, and fluoride synthesis routes were confirmed as crystalline
mordenite framework inverted (MFI) by SEM and XRD and were shown to
contain ∼8.5–0 silanol defects per unit cell by <sup>29</sup>Si MAS, <sup>1</sup>H MAS, and <sup>1</sup>H–<sup>29</sup>Si CPMAS NMR. A hysteresis in the Ar 87 K adsorption isotherm
at 10<sup>–3</sup> <i>P</i>/<i>P</i><sub>0</sub> evolved with a decrease in silanol defects, and, through
features in the XRD and <sup>29</sup>Si MAS NMR spectra, it is postulated
that the hysteresis is the result of an orthorhombic–monoclinic
symmetry shift with decreasing silanol defect density. Gravimetric
and aqueous solution measurements reveal that propylene glycol adsorption
at 333 K is promoted by silanol defects, with a maximum 20-fold increase
observed for aqueous adsorption at ∼10<sup>–3</sup> g/mL
with an increase from ∼0 to 8.5 silanols per unit cell. A comparison
of vapor and aqueous propylene glycol adsorption isotherms on defect-free
silicalite-1 at 333 K, both of which exhibit the Type-V character,
indicates that water enhances adsorption by a factor of ∼2
in the Henry’s Law regime. Henry’s constants for aqueous
C<sub>2</sub>–C<sub>4</sub> polyol adsorption (concentrations
below 0.004 g/mL) at 298 K are shown to have a linear dependence on
the silanol defect density, demonstrating that these molecules preferentially
adsorb at silanol defects at dilute concentrations. This systematic
study of polyol adsorption on silicalite-1 materials highlights the
critical role of defects on adsorption of hydrophilic molecules and
clearly details the effects of coadsorption of water, which can guide
the selection of zeolites for separation of biomass-derived oxygenates
Coating of Open Cell Foams
The interior surfaces of three-dimensional open cell
foams were coated by a combination of dip coating and spin coating.
Glycerol/water solutions were used as model Newtonian liquids, and
the coating processes were studied on open cell carbon foams with
10 or 30 pores per inch (PPI). The amount of liquid retained in the
foam structures after dip coating increased with withdrawal speed
and coating viscosity, as expected from the conventional understanding
of dip coating onto nonporous substrates such as flat plates and rods.
However, the liquid retention and hence average coating thickness
increased with surface tension, a result counter to the observation
with coating onto nonporous substrates. Pockets of liquid were observed
after dip coating and results with coatings of alumina suspension
showed that after drying, the trapped liquid can block pore windows.
Spinning the foams after dip coating resulted in uniform liquid distribution
and uniform coatings. Foams were placed in a special apparatus and
rotated using a commercial spin coater. The liquid layer thickness
decreased with spinning time and rotational speed, and increased with
the liquid viscosity, results consistent with spin coating theory.
The coating thickness after spinning was not affected by the initial
dip coating procedure. The dip and spin process was also used to create
γ-alumina
and zeolite coatings, which are of interest for catalysis applications