10 research outputs found
Porous Carbon Materials Based on Graphdiyne Basis Units by the Incorporation of the Functional Groups and Li Atoms for Superior CO<sub>2</sub> Capture and Sequestration
The
graphdiyne family has attracted a high degree of concern because of
its intriguing and promising properties. However, graphdiyne materials
reported to date represent only a tiny fraction of the possible combinations.
In this work, we demonstrate a computational approach to generate
a series of conceivable graphdiyne-based frameworks (GDY-Rs and Li@GDY-Rs)
by introducing a variety of functional groups (R = −NH<sub>2</sub>, −OH, −COOH, and −F) and doping metal
(Li) in the molecular building blocks of graphdiyne without restriction
of experimental conditions and rapidly screen the best candidates
for the application of CO<sub>2</sub> capture and sequestration (CCS).
The pore topology and morphology and CO<sub>2</sub> adsorption and
separation properties of these frameworks are systematically investigated
by combining density functional theory (DFT) and grand canonical Monte
Carlo (GCMC) simulations. On the basis of our computer simulations,
combining Li-doping and hydroxyl groups strategies offer an unexpected
synergistic effect for efficient CO<sub>2</sub> capture with an extremely
CO<sub>2</sub> uptake of 4.83 mmol/g at 298 K and 1 bar. Combined
with its superior selectivity (13 at 298 K and 1 bar) for CO<sub>2</sub> over CH<sub>4</sub>, Li@GDY-OH is verified to be one of the most
promising materials for CO<sub>2</sub> capture and separation
On the Gas-Phase Co<sup>+</sup>-Mediated Oxidation of Ethane by N<sub>2</sub>O: A Mechanistic Study
The potential energy surface (PES) corresponding to the
Co<sup>+</sup>-mediated oxidation of ethane by N<sub>2</sub>O has
been investigated
by using density functional theory (DFT). After initial N<sub>2</sub>O reduction by Co<sup>+</sup> to CoO<sup>+</sup>, ethane oxidation
by the nascent oxide involves C–H activation followed by two
possible pathways, i.e., C–O coupling accounting for ethanol,
Co<sup>+</sup>-mediated β–H shift giving the energetically
favorable product of CoC<sub>2</sub>H<sub>4</sub><sup>+</sup> + H<sub>2</sub>O, with minor CoOH<sub>2</sub><sup>+</sup> + C<sub>2</sub>H<sub>4</sub>. CoC<sub>2</sub>H<sub>4</sub><sup>+</sup> could react
with another N<sub>2</sub>O to yield (C<sub>2</sub>H<sub>4</sub>)ÂCo<sup>+</sup>O, which could subsequently undergo a cyclization mechanism
accounting for acetaldehyde and oxirane and/or a direct H-abstraction
mechansim for ethenol. Loss of oxirane and ethenol is hampered by
respective endothermicity and high kinetics barrier, whereas acetaldehyde
elimination is much energetically favorable. CoOH<sub>2</sub><sup>+</sup> could facilely react with N<sub>2</sub>O to form OCoOH<sub>2</sub><sup>+</sup>, rather than CoÂ(OH)<sub>2</sub><sup>+</sup> or
CoO<sup>+</sup>
Theoretical Investigation of the Reaction of Mn<sup>+</sup> with Ethylene Oxide
The potential energy surfaces of Mn<sup>+</sup> reaction with ethylene oxide in both the septet and quintet states are investigated at the B3LYP/DZVP level of theory. The reaction paths leading to the products of MnO<sup>+</sup>, MnO, MnCH<sub>2</sub><sup>+</sup>, MnCH<sub>3</sub>, and MnH<sup>+</sup> are described in detail. Two types of encounter complexes of Mn<sup>+</sup> with ethylene oxide are formed because of attachments of the metal at different sites of ethylene oxide, i.e., the O atom and the CC bond. Mn<sup>+</sup> would insert into a C–O bond or the C–C bond of ethylene oxide to form two different intermediates prior to forming various products. MnO<sup>+</sup>/MnO and MnH<sup>+</sup> are formed in the C–O activation mechanism, while both C–O and C–C activations account for the MnCH<sub>2</sub><sup>+</sup>/MnCH<sub>3</sub> formation. Products MnO<sup>+</sup>, MnCH<sub>2</sub><sup>+</sup>, and MnH<sup>+</sup> could be formed adiabatically on the quintet surface, while formation of MnO and MnCH<sub>3</sub> is endothermic on the PESs with both spins. In agreement with the experimental observations, the excited state a<sup>5</sup>D is calculated to be more reactive than the ground state a<sup>7</sup>S. This theoretical work sheds new light on the experimental observations and provides fundamental understanding of the reaction mechanism of ethylene oxide with transition metal cations
Theoretical Investigation of the Methanol Decomposition by Fe<sup>+</sup> and Fe(C<sub>2</sub>H<sub>4</sub>)<sup>+</sup>: A π‑Type Ligand Effect
Density
functional theory has been used to probe the mechanism of gas-phase
methanol decomposition by bare Fe<sup>+</sup> and ligated FeÂ(C<sub>2</sub>H<sub>4</sub>)<sup>+</sup> in both quartet and sextet states.
For the Fe<sup>+</sup>/methanol system, Fe<sup>+</sup> could directly
attach to the O and methyl-H atoms of methanol, respectively, forming
two encounter isomers. The methanol reaction with Fe<sup>+</sup> prefers
initial C–O bond activation to yield methyl with slight endothermicity,
whereas CH<sub>4</sub> elimination is hindered by the strong endothermicity
and high-energy barrier of hydroxyl-H shift. For the FeÂ(C<sub>2</sub>H<sub>4</sub>)<sup>+</sup>/methanol system, the major product of
H<sub>2</sub>O is formed through six elementary steps: encounter complexation,
C–O bond activation, C–C coupling, β-H shift,
hydride H shift, and nonreactive dissociation. Both ligand exchange
and initial C–O bond activation mechanisms could account for
ethylene elimination with the ion products FeÂ(CH<sub>3</sub>OH)<sup>+</sup> and (CH<sub>3</sub>)ÂFeÂ(OH)<sup>+</sup>, respectively. With
the assistance of a π-type C<sub>2</sub>H<sub>4</sub> ligand,
the metal center in the FeÂ(C<sub>2</sub>H<sub>4</sub>)<sup>+</sup>/CH<sub>3</sub>OH system avoids formation of unfavorable multi-σ-type
bonding and thus greatly enhances the reactivity compared to that
of bare Fe<sup>+</sup>
Additional file 1: of Insights into the H2/CH4 Separation Through Two-Dimensional Graphene Channels: Influence of Edge Functionalization
Supporting information. Fig. S1. Final configurations of the 1:1 H2/CH4 mixture permeating through the 2D channel of pristine and edge-functionalized GMs (DOCX 4515 kb
Analysis of Petroleum Aromatics by Laser-Induced Acoustic Desorption/Tunable Synchrotron Vacuum Ultraviolet Photoionization Mass Spectrometry
Laser-induced acoustic desorption
coupled with tunable synchrotron
vacuum ultraviolet photoionization mass spectrometry (LIAD/SVUVPI-MS)
is employed to analyze aromatics prepared under different conditions
from Lungu atmospheric residue (LGAR), i.e., the primary aromatics
separated directly from LGAR, and the secondary aromatics after hydrogenation
of LGAR and its resins. The mass spectra of the primary aromatics
present a bimodal normal distribution in the range of 200–900
Da, in which the relative intensity of the two peaks changes significantly
with the SVUV photon energies (9.0, 11.0, and 14.0 eV), indicating
that at least two categories of compounds with different ionization
energies (IEs) are included, i.e., polycyclic aromatics (IEs <
10.0 eV) in the mass range of 400–900 Da, and aliphatic and
alicyclic compounds (IEs close to 11.0 eV) in 200–400 Da. Also
detected in the aromatics are metalloporphyrins. Furthermore, the
mass spectra of the secondary aromatics separated from LGAR and its
resins at different hydrogenation temperatures (390, 400, 410, and
420 °C) are also recorded. The results indicate that the hydrogenation
process, especially at higher temperatures, results in removal of
alkyl-side and bridge chains in the aromatics, and the secondary aromatics
from LGAR resins contain more alkyl side and bridge chains and metal
compounds than those from LGAR
Theoretical Survey of the Thiophene Hydrodesulfurization Mechanism on Clean and Single-Sulfur-Atom-Modified MoP(001)
Molybdenum
phosphide (MoP) has been extensively experimentally
shown to possess high and surprisingly increasing hydrodesulfurization
(HDS) activities during the HDS process. In order to understand the
HDS mechanism, we investigate the HDS of thiophene on clean and single-sulfur-atom-modified
MoP(001) using self-consistent periodic density functional theory
(DFT). Thiophene strongly prefers <i>flat</i> adsorption,
which is slightly weakened in the presence of a surface S atom. Thermodynamic
and kinetic analyses of the elementary steps show that the HDS of
thiophene takes place along the direct desulfurization (DDS) pathway
on both clean and S-modified MoP(001), because of the very low C–S
bond activation barriers as well as very high exothermicities involved.
More importantly, the surface S atom does not elevate the C–S
bond activation barriers but opens a new concerted pathway for the
simultaneous rupture of both C–S bonds in thiophene. These
results indicate that the presence of a surface S atom could be helpful
for thiophene desulfurization. For comparison, we also investigate
the influence of a surface S atom on the HDS of thiophene on Pt(111).
The results show clearly a negative effect of the surface S atom,
in accordance with the lower sulfur resistance of noble metals
Density Functional Theory Study of the Adsorption and Desulfurization of Thiophene and Its Hydrogenated Derivatives on Pt(111): Implication for the Mechanism of Hydrodesulfurization over Noble Metal Catalysts
Desulfurization of thiophene and its hydrogenated derivatives on Pt(111) are studied using self-consistent periodic density functional theory (DFT), and the hydrodesulfurization network is mapped out. On Pt(111), thiophene has two types of adsorption configurations (parallel cross-bridge and partially tilted bridge-hollow), and for its hydrogenated derivates, the molecule is gradually lifted up from the surface with the addition of hydrogen atoms. In all the adsorbed thiophenic compounds, the S atom is always sp<sup>3</sup> hybridized; the C atom in the methylene group is always sp<sup>3</sup> hybridized, whereas it is either sp<sup>2</sup> or sp<sup>3</sup> hybridized in the methyne group, depending on how the group interacts with the surface Pt atoms. On the basis of the thermodynamic and kinetic analysis of the elementary steps, a direct desulfurization pathway is proposed for the hydrodesulfurization of thiophene on Pt(111). In contrast to the common thought that hydrogenation toward aromatic organosulfur compounds would make desulfurization easier, the present work clearly demonstrates that hydrogenations of thiophene on Pt(111) do not reduce the energy barrier for the C–S bond cleavage
Initial Hydrogenations of Pyridine on MoP(001): A Density Functional Study
The initial hydrogenations of pyridine on MoP(001) with
various
hydrogen species are studied using self-consistent periodic density
functional theory (DFT). The possible surface hydrogen species are
examined by studying interaction of H<sub>2</sub> and H<sub>2</sub>S with the surface, and the results suggest that the rational hydrogen
source for pyridine hydrogenations should be surface hydrogen atoms,
followed by adsorbed H<sub>2</sub>S and SH. On MoP(001), pyridine
has two types of adsorption modes, i.e., side-on and end-on; and the
most stable η<sup>5</sup>(N,C<sup>α</sup>,C<sup>β</sup>,C<sup>β</sup>,C<sup>α</sup>) configuration of the side-on
mode facilitates the hydrogenation of pyridine. The optimal hydrogenation
path of pyridine with surface hydrogen atoms in the Langmuir–Hinshelwood
mechanism is the formation of 3-monohydropyridine, followed by producing
3,5-dihydropyridine, in which the two-step hydrogenations take place
on the C<sup>β</sup> atoms. When adsorbed H<sub>2</sub>S is
considered as the source of hydrogen, slightly higher hydrogenation
barriers are always involved, while the energy barriers for hydrogenations
involving adsorbed SH are much lower. However, the hydrogenation of
pyridine should be suppressed by the adsorption of H<sub>2</sub>S,
and the promotion effect of adsorbed SH is limited
The Competitive O–H versus C–H Bond Activation of Ethanol and Methanol by VO<sub>2</sub><sup>+</sup> in Gas Phase: A DFT Study
The
activation of ethanol and methanol by VO<sub>2</sub><sup>+</sup> in
gas phase has been theoretically investigated by using density functional
theory (DFT). For the VO<sub>2</sub><sup>+</sup>/ethanol system, the
activation energy (Δ<i>E</i>) is found to follow the
order of Δ<i>E</i>(C<sup>β</sup>–H) <
Δ<i>E</i>(C<sup>α</sup>–H) ≈ Δ<i>E</i>(O–H). Loss of methyl and glycol occurs respectively
via O–H and C<sup>β</sup>–H activation, while
acetaldehyde elimination proceeds through two comparable O–H
and C<sup>α</sup>–H activations yielding both VOÂ(H<sub>2</sub>O)<sup>+</sup> and VÂ(OH)<sub>2</sub><sup>+</sup>. Loss of
water not only gives rise to VOÂ(CH<sub>3</sub>CHO)<sup>+</sup> via
both O–H and C<sup>α</sup>–H activation but also
forms VO<sub>2</sub>(C<sub>2</sub>H<sub>4</sub>)<sup>+</sup> via C<sup>β</sup>–H activation. The major product of ethylene
is formed via both O–H and C<sup>β</sup>–H activation
for yielding VOÂ(OH)<sub>2</sub><sup>+</sup> and VO<sub>2</sub>(H<sub>2</sub>O)<sup>+</sup>. In the methanol reaction, both initial O–H
and C<sup>α</sup>–H activation accounts for formaldehyde
and water elimination, but the former pathway is preferred