26 research outputs found
Mechanisms of Mo<sub>2</sub>C(101)-Catalyzed Furfural Selective Hydrodeoxygenation to 2‑Methylfuran from Computation
The selective formation of 2-methylfuran
(F-CH<sub>3</sub>) and
furan from furfural (F-CHO) hydrogenation and hydrodeoxygenation on
clean and 4H precovered Mo<sub>2</sub>CÂ(101) surfaces has been systematically
computed on the basis of periodic density functional theory including
dispersion correction (PBE-D3). The clean Mo<sub>2</sub>CÂ(101) surface
has two distinct surface sites: unsaturated C and Mo sites for the
adsorption of H and furfural, respectively. The selectivity comes
from the different preference of furfural hydrogenation and dissociation
(F-CHO + H = F-CH<sub>2</sub>O vs F-CHO = F-CO + H) under the variation
of H<sub>2</sub> partial pressure. On the basis of the computed minimum
energy path on the clean surface, microkinetics shows that high H<sub>2</sub> partial pressure can promote 2-methylfuran formation and
suppress furan formation. To verify this proposed selectivity trend
of 2-methylfuran at high H<sub>2</sub> partial pressure, the 4H precovered
Mo<sub>2</sub>CÂ(101) surface (0.25 monolayer hydrogen coverage), which
provides neighboring hydrogens for promoting furfural hydrogenation
and blocks the active sites for suppressing furfural dissociation,
has been used. The computed results are in full agreement with the
experimentally observed selective formation of 2-methylfuran and the
H<sub>2</sub> reaction order of one half as well as rationalize the
need for a high H<sub>2</sub>/furfural ratio (400/1). On the basis
of these results, a new two-step protocol for experiments is proposed:
i.e., the first step is the pretreatment of the catalyst with hydrogen,
and the second step is furfural hydrogenation on H precovered catalysts
Mechanisms of CO Activation, Surface Oxygen Removal, Surface Carbon Hydrogenation, and C–C Coupling on the Stepped Fe(710) Surface from Computation
To
understand the initial steps of Fe-based Fischer–Tropsch
synthesis, systematic periodic density functional theory computations
have been performed on the single-atom stepped Fe(710) surface, composed
by <i>p</i>(3 Ă— 3) Fe(100)-like terrace and <i>p</i>(3 Ă— 1) Fe(110)-like step. It is found that CO direct
dissociation into surface C and O is more favored kinetically and
thermodynamically than the H-assisted activation via HCO and COH formation.
Accordingly, surface O removal by hydrogen via H<sub>2</sub>O formation
is the only way. On the basis of surface CH<sub><i>x</i></sub> hydrogenation (<i>x</i> = 0, 1, 2, 3), surface CH<sub><i>x</i></sub> + CH<sub><i>x</i></sub> coupling
and CO + CH<sub><i>x</i></sub> insertion resulting in CH<sub><i>x</i></sub>CO formation followed by C–O dissociation,
surface C hydrogenation toward CH<sub>3</sub> formation is more favored
kinetically than the formation of CH<sub><i>x</i></sub>-CH<sub><i>x</i></sub> and CH<sub><i>x</i></sub>CO, as
well as thermodynamically. Starting from CH<sub>3</sub>, the formation
of CH<sub>4</sub> and CH<sub>3</sub>CO has similar barriers and endothermic
reaction energies, while CH<sub>3</sub>CO dissociation into CH<sub>3</sub>C + O has low barrier and is highly exothermic. Therefore,
turning the H<sub>2</sub>/CO ratio should change the selectivity toward
C–C formation and propagation
Mechanisms of H<sub>2</sub>O and CO<sub>2</sub> Formation from Surface Oxygen Reduction on Co(0001)
Surface
O removal by H and CO on Co(0001) has been studied using
periodic density functional method (revised Perdew–Burke–Ernzerhof
; RPBE) and ab initio atomistic thermodynamics. On the basis of the
quantitative agreement in the H<sub>2</sub>O formation barrier between
experiment (1.34 ± 0.07 eV) and theory (1.32 eV), H<sub>2</sub>O formation undergoes a consecutive hydrogenation process [O + 2H
→ OH + H → H<sub>2</sub>O], while the barrier of H<sub>2</sub>O formation from OH disproportionation [2OH → H<sub>2</sub>O + O] is much lower (0.72 eV). The computed desorption temperatures
of H<sub>2</sub> and H<sub>2</sub>O under ultrahigh vacuum conditions
agree perfectly with the experiment. Surface O removal by CO has a
high barrier (1.41 eV) and is strongly endothermic (0.94 eV). Precovered
O and OH species do not significantly affect the barriers of H<sub>2</sub>O and CO<sub>2</sub> formation. All of these results indicate
that the present RPBE method and the larger surface model are more
suitable for studying cobalt systems
Reactions of CO, H<sub>2</sub>O, CO<sub>2</sub>, and H<sub>2</sub> on the Clean and Precovered Fe(110) Surfaces – A DFT Investigation
The reactions of CO and H<sub>2</sub>O on the clean Fe(110) surface
as well as surfaces with 0.25 monolayer O, OH, and H precoverage have
been computed on the basis of density functional theory (GGA-PBE).
Under the considerations of the reductive nature of CO as reactant
and H<sub>2</sub> as product as well as the oxidative nature of CO<sub>2</sub> and H<sub>2</sub>O, we have studied the potential activity
of metallic iron in the water-gas shift reaction. On the clean surface,
CO oxidation following the redox mechanism has a similar barrier as
CO dissociation; however, CO dissociation is much more favorable thermodynamically.
Furthermore, surfaces with 0.25 monolayer O, OH, and H precoverage
promote CO hydrogenation, while they suppress CO oxidation and dissociation.
On the surfaces with different CO and H<sub>2</sub>O ratios, CO hydrogenation
is promoted. On all of these surfaces, COOH formation is not favorable.
Considering the reverse reaction, CO<sub>2</sub> dissociation is much
favorable kinetically and thermodynamically on all of these surfaces,
and CO<sub>2</sub> hydrogenation should be favorable. Finally, metallic
iron is not an appropriate catalyst for the water-gas shift reaction
Adsorption Structures and Energies of Cu<sub><i>n</i></sub> Clusters on the Fe(110) and Fe<sub>3</sub>C(001) Surfaces
Spin-polarized
density functional theory computations have been
carried out to investigate the adsorption configurations of Cu<sub><i>n</i></sub> (<i>n</i> = 1–7, 13) on
the most stable Fe(110) and Fe<sub>3</sub>CÂ(001) surfaces. On both
surfaces the adsorbed Cu<sub><i>n</i></sub> clusters favor
aggregation over dispersion, and monolayer adsorption configurations
are more favored thermodynamically than the two-layer adsorbed structures
because of the stronger Fe–Cu interaction over the Cu–Cu
bonding. On the basis of the computed adsorption energies the Fe(110)
surface has stronger Cu affinity than the Fe<sub>3</sub>CÂ(001) surface,
in agreement with the experimental results. The Fe(110) surface also
has stronger Cu<sub><i>n</i></sub> aggregation energies
and more pronounced charge transfer from surface to adsorbed Cu<sub><i>n</i></sub> clusters than the Fe<sub>3</sub>CÂ(001) surface.
Different Cu<sub><i>n</i></sub> growth modes have been discussed
accordingly
DFT+U Study of Molecular and Dissociative Water Adsorptions on the Fe<sub>3</sub>O<sub>4</sub>(110) Surface
Spin-polarized
density functional theory method (GGA+U) and periodic
supercell model have been used to study water adsorption properties
on the Fe<sub>3</sub>O<sub>4</sub>(110) surface, which has A and B
terminations in close surface energy. The adsorption of one and two
water molecules is molecular on the A termination, while dissociative
on the B termination. For the adsorption of three and four water molecules,
mixed dissociative and molecular coadsorption is preferred on the
A termination, and fully dissociative adsorption as well as mixed
molecular and dissociative coadsorptions are preferred on the B terminations.
The stepwise adsorption energies show that the full monolayer water
adsorption on both terminations is thermodynamically possible. Further
analysis shows that surface iron atoms and hydrogen bonding contribute
to the adsorption energies. The adsorption mechanism has been analyzed
on the basis of projected density of states (PDOS)
Dissociative Hydrogen Adsorption on the Hexagonal Mo<sub>2</sub>C Phase at High Coverage
Hydrogen
adsorption on the primarily exposed (001), (100), (101), and (201)
surfaces of the hexagonal Mo<sub>2</sub>C phase at different coverage
has been investigated at the level of density functional theory and
using ab initio thermodynamics. On the Mo-terminated (001) and (100)
as well as mixed Mo/C-terminated (101) and (201) surfaces, dissociative
H<sub>2</sub> adsorption is favored both kinetically and thermodynamically.
At high coverage, each surface can have several types of adsorption
configurations coexisting, and these types are different from surface
to surface. The stable coverage as a function of temperature and partial
pressure provides useful information not only for surface science
studies at ultrahigh vacuum condition but also for practical applications
at high temperature and pressure in monitoring reactions. The differences
in the adsorbed H atom numbers and energies of these surfaces indicate
their different potential hydrotreating abilities. The relationship
between surface stability and stable hydrogen coverage has been discussed
Adsorption Equilibria of CO Coverage on β-Mo<sub>2</sub>C Surfaces
Adsorption and surface coverage of CO on the (001), (101),
and
(201) surfaces of β-Mo<sub>2</sub>C were computed at the level
of density functional theory under the consideration of the temperature
and CO partial pressure by using the ab initio atomistic thermodynamic
method. On the basis of the computed Gibbs free energies, the relationship
between CO coverage on the surfaces and temperature as well as CO
partial pressure has been established, and excellent agreements have
been found between the predicated CO desorption temperatures and the
experimentally recorded temperature programmed desorption (TPD) spectra.
These computed phase diagrams show that a stable CO coverage can be
obtained within a range of temperature and partial pressure; different
surfaces can have different coverage at the same conditions, and different
partial pressure has a different desorption temperature. In addition,
these phase diagrams provide useful information for adjusting the
balance between temperature and CO partial pressure for a stable CO
coverage and for identifying the active surface and the initial states
under given conditions. These results should also be very interesting
for surface science under ultra high vacuum conditions
Exploring Furfural Catalytic Conversion on Cu(111) from Computation
The full potential energy surface
of the catalytic conversion of
furfural to 2-methylfuran on the Cu(111) surface has been systematically
computed on the basis of density functional theory, including dispersion
and zero-point energy corrections. For furfuryl alcohol formation,
the more favorable step is the first H addition to the carbon atom
of the Cî—»O group, forming an alkoxyl intermediate (F-CHO +H
→ F-CH<sub>2</sub>O); the second H atom addition, leading to
furfuryl alcohol formation (F-CH<sub>2</sub>O + H → F-CH<sub>2</sub>OH), is the rate-determining step. For 2-methylfuran formation
from furfuryl alcohol dissociation into surface alkyl (F-CH<sub>2</sub>) and OH groups, H<sub>2</sub>O formation is the rate-determining
step (OH + H → H<sub>2</sub>O). Our results explain perfectly
the experimentally observed selective formation of furfuryl alcohol
and the equilibrium of furfural/furfuryl alcohol conversion under
hydrogen-rich conditions as well as the effect of H<sub>2</sub>O suppressing
furfural conversion. In addition, it is found that dispersion correction
(PBE-D3) overestimates the adsorption energies of furfural, furfuryl
alcohol, and 2-methylfuran considerably, whereas those of H<sub>2</sub> and H<sub>2</sub>O can be reproduced nearly quantitatively. Our
results provide insights into Cu-catalyzed furfural selective conversion
and broaden our fundamental understanding into deoxygenation reactions
of oxygenates involved in the refining of biomass-derived oils
Copper Promotion in CO Adsorption and Dissociation on the Fe(100) Surface
Spin-polarized density functional
theory computations have been carried out to study the adsorption
and dissociation of CO on clean as well as <i>n</i>Cu-adsorbed
and <i>n</i>Cu-substituted Fe(100) surfaces (<i>n</i> = 1–3) at different coverage to explore the Cu promotion
effect in CO activation. Increasing Cu content not only lowers CO
dissociation energies but also increases CO dissociation barriers
as well as making CO dissociation thermodynamically less favorable,
and the clean Fe(100) surface is most active in CO adsorption and
dissociation. The <i>n</i>Cu-substituted Fe(100) surface
can suppress CO adsorption and dissociation more strongly than the <i>n</i>Cu-adsorbed Fe(100) surface. CO stretching frequencies
at different coverages have been computed for assisting experimental
investigations