40 research outputs found
Aerobic Oxidation of Formaldehyde Catalyzed by Polyvanadotungstates
Three tetra-<i>n</i>-butylammonium
(TBA) salts of polyvanadotungstates,
[<i>n</i>-Bu<sub>4</sub>N]<sub>6</sub>[PW<sub>9</sub>V<sub>3</sub>O<sub>40</sub>] (<b>PW</b><sub><b>9</b></sub><b>V</b><sub><b>3</b></sub>), [<i>n</i>-Bu<sub>4</sub>N]<sub>5</sub>H<sub>2</sub>PW<sub>8</sub>V<sub>4</sub>O<sub>40</sub> (<b>PW</b><sub><b>8</b></sub><b>V</b><sub><b>4</b></sub>), and [<i>n</i>-Bu<sub>4</sub>N]<sub>4</sub>H<sub>5</sub>PW<sub>6</sub>V<sub>6</sub>O<sub>40</sub>·20H<sub>2</sub>O (<b>PW</b><sub><b>6</b></sub><b>V</b><sub><b>6</b></sub>), have been synthesized and shown to be effective
catalysts for the aerobic oxidation of formaldehyde to formic acid
under ambient conditions. These complexes, characterized by elemental
analysis, Fourier transform infrared spectroscopy, UV–vis spectroscopy,
and thermogravimetric analysis, exhibit a catalytic activity for this
reaction comparable to those of other polyoxometalates. Importantly,
they are more effective in the presence of water than the metal oxide-supported
Pt and/or Au nanoparticles traditionally used as catalysts for formaldehyde
oxidation in the gas phase. The polyvanadotungstate-catalyzed oxidation
reactions are first-order in formaldehyde, parabolic-order (slow,
fast, and slow again) in catalyst, and zero-order in O<sub>2</sub>. Under optimized conditions, a turnover number of ∼57 has
been obtained. These catalysts can be recycled and reused without
a significant loss of catalytic activity
A Hybrid Quantum Mechanical Approach: Intimate Details of Electron Transfer between Type‑I CdSe/ZnS Quantum Dots and an Anthraquinone Molecule
We
report a hybrid computational approach to calculate electron
transfer between a type-I CdSe/ZnS core/shell quantum dot (QD) with
a varying shell thickness and the functionalized anthraquinone (AQ)
molecule. This novel approach combines the traditional electron/hole
confinement theory in the effective mass approximation for the QD
and molecular orbital theory for the AQ molecule. In the present study,
the QD’s electron and hole envelope wave functions are solutions
of the effective-mass Schrödinger equation, and the AQ wave
function is obtained at the density functional level. Electron-transfer
rate calculations are based on Marcus’s theory with the coupling
strength computed according to an one-electron orbital perturbation
model. We show that in a heptane solution, the LUMO of AQ and the
1S<sub>e</sub> electron orbital of QD are involved in the charge separation
(CS) process. The charge recombination (CR) process, on the other
hand, occurs from the singly occupied molecular orbital of the AQ
radical (which corresponds to the LUMO in AQ) to a trapped hole state
of the QD within the band gap. The calculations support previously
reported interpretations of the role of the ZnS shell as a hindrance
in the CS and CR process
Synergetic Catalysis of Copper and Iron in Oxidation of Reduced Keggin Heteropolytungstates by Dioxygen
Polyoxometalates
(POMs) and in particularly Keggin heteropolytungstates
are much studied and commercially important catalysts for dioxygen-based
oxidation processes. The rate-limiting step in many POM-catalyzed
O<sub>2</sub>-based oxidations is reoxidation of the reduced POM by
O<sub>2</sub>. We report here that this reoxidation process, as represented
by the one-electron-reduced Keggin complexes POM<sub>red</sub> (α-PW<sub>12</sub>O<sub>40</sub><sup>4–</sup> and α-SiVW<sub>11</sub>O<sub>40</sub><sup>6–</sup>) reacting with O<sub>2</sub>,
is efficiently catalyzed by a combination of copper and iron complexes.
The reaction kinetics and mechanism have been comprehensively studied
in sulfate and phosphate buffer at pH 1.8. The catalytic pathway includes
a reversible reaction between CuÂ(II) and FeÂ(II), followed by a fast
oxidation of POM<sub>red</sub> by FeÂ(III) and CuÂ(I) by O<sub>2</sub> to regenerate FeÂ(II) and CuÂ(II). The proposed reaction mechanism
quantitatively describes the experimental kinetic curves over a wide
range of experimental conditions. Since the oxidized forms, α-PW<sub>12</sub>O<sub>40</sub><sup>3–</sup> and α-SiVW<sub>11</sub>O<sub>40</sub><sup>5–</sup>, are far better oxidants of organic
substrates than the previously studied POMs, α-SiW<sub>12</sub>O<sub>40</sub><sup>4–</sup> and α-AlW<sub>12</sub>O<sub>40</sub><sup>5–</sup>, this synergistic Fe/Cu cocatalysis
of reduced-POM reoxidation could well facilitate significant new O<sub>2</sub>/air-based processes
Reaction Mechanism of Nerve-Agent Hydrolysis with the Cs<sub>8</sub>Nb<sub>6</sub>O<sub>19</sub> Lindqvist Hexaniobate Catalyst
We
present a detailed mechanism for the hydrolysis of Sarin catalyzed
by Cs<sub>8</sub>Nb<sub>6</sub>O<sub>19</sub> obtained using electronic
structure calculations. The initial steps of the reaction involve
the adsorption of water and Sarin on the hexaniobate catalyst via
nonbonding interactions. Dissociation of the coordinated water molecule
generates a hydroxide ion that adds nucleophilically to the coadsorbed
Sarin molecule in a concerted manner, following a general base catalysis
mechanism. The addition of OH<sup>–</sup> to the nerve agent
generates a trigonal bipyramidal pentacoordinated phosphorus intermediate
that subsequently undergoes facile dissociation forming either HF
or isopropanol and a corresponding phosphonic acid. The rate-determining
step of the overall reaction is found to be the dissociation of water
on the catalyst in concert with the nucleophilic addition of the nascent
OH<sup>–</sup> to the nerve agent. The calculated barrier for
this step is considerably smaller than that measured for bulk base
hydrolysis. This work represents a blueprint for future studies aimed
to optimize catalysts for base hydrolysis of nerve agents at the gas–surface
interface
Structural Modification of TiO<sub>2</sub> Surfaces in Bulk Water and Binding Motifs of a Functionalized C<sub>60</sub> on TiO<sub>2</sub> Anatase and Rutile Surfaces in Vacuo and in Water: Molecular Dynamics Studies
The nature of several TiO<sub>2</sub> surfaces in liquid
water,
as well as the adsorption of a functionalized C<sub>60</sub>, <b>L*C</b><sub><b>60</b></sub> (where L is a carboxylic acid),
on TiO<sub>2</sub> anatase and rutile low index surfaces in vacuo
and in liquid water have been studied at the self-consistent charge
density functional tight-binding (SCC-DFTB) level of theory. It is
shown that the SCC-DFTB method provides very good agreement with the
high-level DFT data. The typical binding motif of <b>L*C</b><sub><b>60</b></sub><b>@TiO</b><sub><b>2</b></sub> is found to be the formation of a strong HC<sup>1</sup>CÂ(O<sup>2</sup>H)ÂO<sup>1</sup>–Ti<sub>5C</sub>/O<sup>1</sup>–Ti<sub>4C</sub> bond with a distance of 2.0–2.1 Ã… and a weaker
HC<sup>1</sup>CO<sup>1</sup>O<sup>2</sup>–H···O<sub>2C</sub>/O<sup>2</sup>···H–O<sub>2C</sub> hydrogen
bond. In some cases, a terminal OH of the linking group coordinates
with a Ti–O–Ti bridging oxygen and loses the H to the
surface. The adsorption energies in vacuum range between 21 and 82
kcal/mol depending on the surface. The density of states of these
species reveals the presence of peaks below the surface conduction
band upon ligand adsorption, which is due to the low-lying lowest
unoccupied molecular orbitals (LUMOs) of the <b>L*C</b><sub><b>60</b></sub>. Electron transfer from the surface to the
ligand is thus possible via the initial UV photoexcitation of the
surface followed by nonradiative relaxation of the excited electron
to the LUMO of the ligand. This pattern was observed for all six surfaces
considered in the present work. Solvation of <b>C</b><sub><b>60</b></sub><b>@TiO</b><sub><b>2</b></sub> in liquid
water does not change the qualitative character of surface–ligand
binding. In all cases, the ligand remains bound to the surface in
the presence of water. The interaction of water molecules with the
surface shows various patterns depending on the surface index. Anatase
(101) and (100) surfaces favor nondissociative water adsorption, while
anatase (001) and rutile (001), (110), and (101) surfaces show dissociative
water adsorption which results in OH/OH<sub>2</sub>-terminated TiO<sub>2</sub> surfaces. The latter finding is in agreement with several
previous DFT studies reported by others
Reaction Mechanism of Nerve-Agent Hydrolysis with the Cs<sub>8</sub>Nb<sub>6</sub>O<sub>19</sub> Lindqvist Hexaniobate Catalyst
We
present a detailed mechanism for the hydrolysis of Sarin catalyzed
by Cs<sub>8</sub>Nb<sub>6</sub>O<sub>19</sub> obtained using electronic
structure calculations. The initial steps of the reaction involve
the adsorption of water and Sarin on the hexaniobate catalyst via
nonbonding interactions. Dissociation of the coordinated water molecule
generates a hydroxide ion that adds nucleophilically to the coadsorbed
Sarin molecule in a concerted manner, following a general base catalysis
mechanism. The addition of OH<sup>–</sup> to the nerve agent
generates a trigonal bipyramidal pentacoordinated phosphorus intermediate
that subsequently undergoes facile dissociation forming either HF
or isopropanol and a corresponding phosphonic acid. The rate-determining
step of the overall reaction is found to be the dissociation of water
on the catalyst in concert with the nucleophilic addition of the nascent
OH<sup>–</sup> to the nerve agent. The calculated barrier for
this step is considerably smaller than that measured for bulk base
hydrolysis. This work represents a blueprint for future studies aimed
to optimize catalysts for base hydrolysis of nerve agents at the gas–surface
interface
Reaction Mechanism of Nerve-Agent Hydrolysis with the Cs<sub>8</sub>Nb<sub>6</sub>O<sub>19</sub> Lindqvist Hexaniobate Catalyst
We
present a detailed mechanism for the hydrolysis of Sarin catalyzed
by Cs<sub>8</sub>Nb<sub>6</sub>O<sub>19</sub> obtained using electronic
structure calculations. The initial steps of the reaction involve
the adsorption of water and Sarin on the hexaniobate catalyst via
nonbonding interactions. Dissociation of the coordinated water molecule
generates a hydroxide ion that adds nucleophilically to the coadsorbed
Sarin molecule in a concerted manner, following a general base catalysis
mechanism. The addition of OH<sup>–</sup> to the nerve agent
generates a trigonal bipyramidal pentacoordinated phosphorus intermediate
that subsequently undergoes facile dissociation forming either HF
or isopropanol and a corresponding phosphonic acid. The rate-determining
step of the overall reaction is found to be the dissociation of water
on the catalyst in concert with the nucleophilic addition of the nascent
OH<sup>–</sup> to the nerve agent. The calculated barrier for
this step is considerably smaller than that measured for bulk base
hydrolysis. This work represents a blueprint for future studies aimed
to optimize catalysts for base hydrolysis of nerve agents at the gas–surface
interface
Oxidation of Reduced Keggin Heteropolytungstates by Dioxygen in Water Catalyzed by Cu(II)
The reaction of reduced polyoxometalates
(POMs) with dioxygen is centrally important in POM catalysis. We report
that this process, as represented by the one-electron-reduced Keggin
complexes POM<sub>red</sub> (α-AlW<sub>12</sub>O<sub>40</sub><sup>6–</sup>, α-SiW<sub>12</sub>O<sub>40</sub><sup>5–</sup>, and α-PW<sub>12</sub>O<sub>40</sub><sup>4–</sup>), is efficiently catalyzed by copper complexes. The Cu-catalyzed
pathway is dominant in the presence of as low as ∼0.1 μM
of Cu, a copper concentration that is typically lower than the copper
ion contamination in aqueous solutions. The reaction kinetics and
mechanism have been comprehensively studied in sodium sulfate buffer
at pH 2.0. The catalytic pathway includes a reversible reduction of
CuÂ(II) by POM<sub>red</sub>, followed by a fast reoxidation of CuÂ(I)
by O<sub>2</sub> to regenerate CuÂ(II). The rate constants of the first
catalytic steps were determined by three approaches and found to be
(1.8 ± 0.3) × 10<sup>5</sup> and 57 ± 15 M<sup>–1</sup> s<sup>–1</sup> for SiW<sub>12</sub>O<sub>40</sub><sup>5–</sup> and PW<sub>12</sub>O<sub>40</sub><sup>4–</sup>, respectively.
These reactions are thermodynamically more favorable and therefore
proceed significantly more quickly than those for the direct outer-sphere
electron transfer to O<sub>2</sub>. The proposed reaction mechanism
quantitatively describes the experimental kinetic curves over a wide
range of experimental conditions
Parameterization of Reactive Force Field: Dynamics of the [Nb<sub>6</sub>O<sub>19</sub>H<sub><i>x</i></sub>]<sup>(8–<i>x</i>)–</sup> Lindqvist Polyoxoanion in Bulk Water
We present results on parameterization
of reactive force field
[van Duin, A. C. T.; Dasgupta, S.; Lorant, F.; Goddard, W. A. ReaxFF:
A Reactive Force Field for Hydrocarbons. <i>J. Phys. Chem. A</i> <b>2001</b>, <i>105</i>, 9396–9409] for investigating
the properties of the [Nb<sub>6</sub>O<sub>19</sub>H<sub><i>x</i></sub>]<sup>(8–<i>x</i>)–</sup> Lindqvist
polyoxoanion, <i>x</i> = 0–8, in water. Force-field
parameters were fitted to an extensive data set consisting of structures
and energetics obtained at the Perdew–Burke–Ernzerhof
density functional level of theory. These parameters can reasonably
describe pure water structure as well as water with an excess of H<sup>+</sup> and OH<sup>–</sup> ions. Molecular dynamics simulations
were performed on [Nb<sub>6</sub>O<sub>19</sub>H<sub><i>x</i></sub>]<sup>(8–<i>x</i>)–</sup>, <i>x</i> = 0–8, submerged in bulk water at 298 K. Analysis
of the MD trajectories showed facile H atom transfer between the protonated
polyoxoanion core and bulk water. The number of oxygen sites labeled
with an H atom was found to vary depending on the pH of the solution.
Detailed analysis shows that the total number of protons at bridging
(terminal), η-O (μ<sub>2</sub>-O), sites ranges from 3(1)
at pH 7, to 2(0) at pH 11, to 1(0) at pH 15. These findings closely
reflect available experimental measurements
Near Unity Quantum Yield of Light-Driven Redox Mediator Reduction and Efficient H<sub>2</sub> Generation Using Colloidal Nanorod Heterostructures
The advancement of direct solar-to-fuel conversion technologies
requires the development of efficient catalysts as well as efficient
materials and novel approaches for light harvesting and charge separation.
We report a novel system for unprecedentedly efficient (with near-unity
quantum yield) light-driven reduction of methylviologen (MV<sup>2+</sup>), a common redox mediator, using colloidal quasi-type II CdSe/CdS
dot-in-rod nanorods as a light absorber and charge separator and mercaptopropionic
acid as a sacrificial electron donor. In the presence of Pt nanoparticles,
this system can efficiently convert sunlight into H<sub>2</sub>, providing
a versatile redox mediator-based approach for solar-to-fuel conversion.
Compared to related CdSe seed and CdSe/CdS core/shell quantum dots
and CdS nanorods, the quantum yields are significantly higher in the
CdSe/CdS dot-in-rod structures. Comparison of charge separation, recombination
and hole filling rates in these complexes showed that the dot-in-rod
structure enables ultrafast electron transfer to methylviologen, fast
hole removal by sacrificial electron donor and slow charge recombination,
leading to the high quantum yield for MV<sup>2+</sup> photoreduction.
Our finding demonstrates that by controlling the composition, size
and shape of quantum-confined nanoheterostructures, the electron and
hole wave functions can be tailored to produce efficient light harvesting
and charge separation materials