19 research outputs found
Mechanistic Investigation of the Catalytic Decomposition of Ammonia (NH<sub>3</sub>) on an Fe(100) Surface: A DFT Study
Catalytic decomposition of ammonia
(NH<sub>3</sub>) is a promising chemical reaction in energy and environmental
applications. Density functional theory (DFT) calculations were performed
to clarify the detailed catalytic mechanism of NH<sub>3</sub> decomposition
on an Fe(100) surface. Specifically, the elementary steps of the mechanism
were calculated for the general dehydrogenation pathway of NH<sub>3</sub>. The adsorption of two types of ammonia dimers (2NH<sub>3</sub>), locally adsorbed NH<sub>3</sub> and hydrogen-bonded NH<sub>3</sub>, were then compared, revealing that locally adsorbed NH<sub>3</sub> is more stable than hydrogen-bonded NH<sub>3</sub>. By contrast,
the dehydrogenation of dimeric NH<sub>3</sub> results in a high energy
barrier. Moreover, the catalytic characteristics of NH<sub>3</sub> decomposition on a nitrogen (N)-covered Fe surface must be considered
because the recombination of nitrogen (N<sub>2</sub>) and desorption
have an extremely high energy barrier. Our results indicate that the
catalytic characteristics of the NH<sub>3</sub> decomposition reaction
are altered by N coverage of the Fe surface. This study primarily
focused on energetic and electronic analysis. Finally, we conclude
that Fe is an alternative catalyst for the decomposition of NH<sub>3</sub> in CO<sub><i>x</i></sub>-free hydrogen production
Interpenetration of Metal Organic Frameworks for Carbon Dioxide Capture and Hydrogen Purification: Good or Bad?
Using grand canonical Monte Carlo (GCMC) simulations
with our recently
developed first-principles-based force fields, we report the effects
of porosity and interpenetration on the CO<sub>2</sub> uptake in 14
prototypical MOFs (metal organic frameworks). The maximum CO<sub>2</sub> capacity for both total and excess uptakes at high pressures (e.g.,
50 bar) correlates well with the pore volume of MOFs and zeolitic
imidazolate frameworks, rather than the surface area, which agrees
well with the experimental results. The interpenetration between MOFs
leads to smaller pore volume (higher density) lowering the maximum
CO<sub>2</sub> uptake at high pressures. However, the interpenetrating
MOFs produce new CO<sub>2</sub> adsorption sites with high binding
affinity (approximately twice that of noninterpenetrating MOFs), such
as shared spaces created by two organic linkers of adjacent MOFs,
enhancing CO<sub>2</sub> uptake at low pressures (e.g., 2 bar). For
H<sub>2</sub> uptake at 298 K, on the other hand, the interpenetration
does not provide positive effects. For these reasons, the interpenetration
of MOFs remarkably enhances the selectivity of CO<sub>2</sub> over
H<sub>2</sub>, by more than 3 times that of noninterpenetrating MOFs.
These results also show that smaller pores in MOFs are, indeed, advantageous
for the CO<sub>2</sub>/H<sub>2</sub> separation
ReaxFF Molecular Dynamics Simulations of Water Stability of Interpenetrated MetalāOrganic Frameworks
Molecular dynamics
(MD) simulations using the reactive force field
(ReaxFF) have been performed to elucidate the underlying water-induced
disruption mechanism of several prototypical interpenetrated MOFs
(IRMOF-9, IRMOF-13, and SUMOF-4). Through the comparison to the corresponding
noninterpenetrated MOFs (IRMOF-10 and IRMOF-14), for both the interpenetrated
and noninterpenetrated MOFs, structural collapse was always accompanied
by the dissociation of the water molecules, with the produced OH<sup>ā</sup> and H<sup>+</sup> forming chemical bonds with the
Zn<sup>2+</sup> ion and O atom of the ligand, respectively. However,
the water stability of the interpenetrated MOFs is less than that
of the corresponding noninterpenetrated structures. The reasons for
the differences between the MOFs in the resistance to water attack
are clarified. The water resistance of the noninterpenetrated MOFs
is mainly attributed to the strength of the ZnāO<sub>ligand</sub>, but, the hydrogen bond has little effect. However, a trade-off
between the strength of the ZnāO<sub>ligand</sub> bond and
the hydrogen bond determines the water stability of the interpenetrated
MOFs. We expect that our understanding of the water-disruption mechanisms
of MOFs will provide helpful guidance for the design of MOFs with
a high water-resistance. Additionally, this work shows that ReaxFF
simulations could be a useful technique for predicting the hydrothermal
stability of MOFs
High H<sub>2</sub> Uptake in Li-, Na-, K-Metalated Covalent Organic Frameworks and Metal Organic Frameworks at 298 K
The Yaghi laboratory has developed porous covalent organic frameworks (COFs), COF102, COF103, and COF202, and metalāorganic frameworks (MOFs), MOF177, MOF180, MOF200, MOF205, and MOF210, with ultrahigh porosity and outstanding H<sub>2</sub> storage properties at 77 K. Using grand canonical Monte Carlo (GCMC) simulations with our recently developed first principles based force field (FF) from accurate quantum mechanics (QM), we calculated the molecular hydrogen (H<sub>2</sub>) uptake at 298 K for these systems, including the uptake for Li-, Na-, and K-metalated systems. We report the total, delivery and excess amount in gravimetric and volumetric units for all these compounds. For the gravimetric delivery amount from 1 to 100 bar, we find that eleven of these compounds reach the 2010 DOE target of 4.5 wt % at 298 K. The best of these compounds are MOF200-Li (6.34) and MOF200-Na (5.94), both reaching the 2015 DOE target of 5.5 wt % at 298 K. Among the undoped systems, we find that MOF200 gives a delivery amount as high as 3.24 wt % while MOF210 gives 2.90 wt % both from 1 to 100 bar and 298 K. However, none of these compounds reach the volumetric 2010 DOE target of 28 g H<sub>2</sub>/L. The best volumetric performance is for COF102-Na (24.9), COF102-Li (23.8), COF103-Na (22.8), and COF103-Li (21.7), all using delivery g H<sub>2</sub>/L units for 1ā100 bar. These are the highest volumetric molecular hydrogen uptakes for a porous material under these thermodynamic conditions. Thus, one can obtain outstanding H<sub>2</sub> uptakes with Li, Na, and K doping of simple frameworks constructed from simple, cheap organic linkers. We present suggestions for strategies for synthesis of alkali metal-doped MOFs or COFs
Tuning MetalāOrganic Frameworks with Open-Metal Sites and Its Origin for Enhancing CO<sub>2</sub> Affinity by Metal Substitution
Reducing anthropogenic carbon emission is a problem that
requires
immediate attention. Metalāorganic frameworks (MOFs) have emerged
as a promising new materials platform for carbon capture, of which
Mg-MOF-74 offers chemospecific affinity toward CO<sub>2</sub> because
of the open Mg sites. Here we tune the binding affinity of CO<sub>2</sub> for M-MOF-74 by metal substitution (M = Mg, Ca, and the first
transition metal elements) and show that Ti- and V-MOF-74 can have
an enhanced affinity compared to Mg-MOF-74 by 6ā9 kJ/mol. Electronic
structure calculations suggest that the origin of the major affinity
trend is the local electric field effect of the open metal site that
stabilizes CO<sub>2</sub>, but forward donation from the lone-pair
electrons of CO<sub>2</sub> to the empty d-levels of transition metals
as in a weak coordination bond makes Ti and V have an even higher
binding strength than Mg, Ca, and Sc
Correction and Addition to āTuning MetalāOrganic Frameworks with Open-Metal Sites and Its Origin for Enhancing CO<sub>2</sub> Affinity by Metal Substitutionā
Correction and Addition
to āTuning MetalāOrganic Frameworks with Open-Metal
Sites and Its Origin for Enhancing CO<sub>2</sub> Affinity by Metal
Substitution
High-Throughput Screening to Investigate the Relationship between the Selectivity and Working Capacity of Porous Materials for Propylene/Propane Adsorptive Separation
An efficient propylene/propane separation
is a very critical process
for saving the cost of energy in the petrochemical industry. For separation
based on the pressure-swing adsorption process, we have screened ā¼1
million crystal structures in the Cambridge Structural Database and
Inorganic Crystal Structural Database with descriptors such as the
surface area of N<sub>2</sub>, accessible surface area of propane,
and pore-limiting diameter. Next, grand canonical Monte Carlo simulations
have been performed to investigate the selectivities and working capacities
of propylene/propane under experimental process conditions. Our simulations
reveal that the selectivity and the working capacity have a trade-off
relationship. To increase the working capacity of propylene, porous
materials with high largest cavity diameters (LCDs) and low propylene
binding energies (<i>Q</i><sub>st</sub>) should be considered;
conversely, for a high selectivity, porous materials with low LCDs
and high propylene <i>Q</i><sub>st</sub> should be considered,
which leads to a trade-off between the selectivity and the working
capacity. In addition, for the design of novel porous materials with
a high selectivity, we propose a porous material that includes elements
with a high crossover distance in their Lennard-Jones potentials for
propylene/propane such as In, Te, Al, and I, along with the low LCD
stipulation
Direct Synthesis of Hydrogen Peroxide from Hydrogen and Oxygen over Mesoporous Silica-Shell-Coated, Palladium-Nanocrystal-Grafted SiO<sub>2</sub> Nanobeads
Many
studies have been conducted on coreāshell structured
nanocatalysts thanks to their high thermal and physical stability.
However, for a typical coreāshell structure, shell thickness
and pore size that affect mass transfer through the shell are difficult
to control. Herein, we synthesized a different type of coreāshell
catalyst, in which a mesoporous silica shell encapsulates the Pd-nanocrystals-grafted-SiO<sub>2</sub> nanobeads. With the preparation method introduced, we successfully
controlled the thickness of the shell layer and generated a mesoporous
texture over the shell layer. In activity tests, the production rate
of hydrogen peroxide significantly increased when using the mesoporous
shell catalyst over the microporous shell catalyst of similar shell
thickness. The thickening of the mesoporous shell layer reduced the
production rate of hydrogen peroxide. Thus, the thinner the thickness
of a mesoporous shell, the more favorable in terms of pore-diffusion
rate. However, the shell thickness should be adequately adjusted,
because an extremely thin shell layer cannot protect the core Pd crystals
from thermal agglomeration in a calcination and reduction process
Activity, Selectivity, and Durability of Ruthenium Nanoparticle Catalysts for Ammonia Synthesis by Reactive Molecular Dynamics Simulation: The Size Effect
We
report a molecular dynamics (MD) simulation employing the reactive
force field (ReaxFF), developed from various first-principles calculations
in this study, on ammonia (NH<sub>3</sub>) synthesis from nitrogen
(N<sub>2</sub>) and hydrogen (H<sub>2</sub>) gases over Ru nanoparticle
(NP) catalysts. Using ReaxFF-MD simulations, we predict not only the
activities and selectivities but also the durabilities of the nanocatalysts
and discuss the size effect and process conditions (temperature and
pressure). Among the NPs (diameter = 3, 4, 5, and 10 nm) considered
in this study, the 4 nm NPs show the highest activity, in contrast
to our intuition that the smallest NP should provide the highest activity,
as it has the highest surface area. In addition, the best selectivity
is observed with the 10 nm NPs. The activity and selectivity are mainly
determined by the hcp, fcc, and top sites on the Ru NP surface, which
depend on the NP size. Moreover, the selectivity can be improved more
significantly by increasing the H<sub>2</sub> pressure than by increasing
the N<sub>2</sub> pressure. The durability of the NPs can be determined
by the mean stress and the stress concentration, and these two factors
have a trade-off relationship with the NP size. In other words, as
the NP size increases, its mean stress decreases, whereas the stress
concentration simultaneously increases. Because of these two effects,
the best durability is found with the 5 nm NPs, which is also in contrast
to our intuition that larger NPs should show better durability. We
expect that ReaxFF-MD simulations, along with first-principles calculations,
could be a useful tool in developing novel catalysts and understanding
catalytic reactions
Band Gap Engineering of Paradigm MOFā5
Recently, metalāorganic frameworks
(MOFs) have demonstrated
great potential in photocatalysis and luminosity applications. However,
most MOFs are dielectrics with substantial band gaps which limits
applications of MOFs in the visible-light region. In this paper, we
systematically tune the band gap of paradigm MOF-5 by substituting
new atoms for the corner elements (X<sub>4</sub>Y), in computer simulations
using density functional theory. The new proposed materials are labeled
X<sub>4</sub>YāMOF-5 (X = Zn, Cd, Be, Mg, Ca, Sr, Ba; Y = O,
S, Se, Te). These new materials have band gaps ranging from 1.7 to
3.6 eV. The underlying mechanism of tunability of band gap can be
ascribed to the electronic states of chalcogen atoms (O, S, Se, Te)
in the X<sub>4</sub>Y nodes and carbon atoms in the BDC linkers. The
substantial tunability of band gap leads to a large absorption range
covering the visible spectrum. These proposed new materials may be
useful for future applications in visible-light promoted photocatalysis
or luminosity. The tunability of other properties such as bulk modulus,
chemical bonding, and optical properties were also investigated. These
novel materials may also be useful for devices in nanoelectronics
or optoelectronics