14 research outputs found
Modifying the Fullerene Surface Using Endohedral Noble Gas Atoms: Density Functional Theory Based Molecular Dynamics Study of C<sub>70</sub>O<sub>3</sub>
We have performed a series of ab initio molecular orbital and molecular
dynamics calculations to ascertain the influence of an endohedral
noble gas atom on the reactivity of the surface of the model system
C<sub>70</sub>O<sub>3</sub>. Our simulations show that the minimum
energy pathways for the ozone ring-opening reaction are influenced
by the presence of the endohedral atom. The effect is isomer dependent,
with the enthalpy of the reaction increasing for <i>a</i>,<i>b</i>-C<sub>70</sub>O<sub>3</sub> and decreasing for <i>e</i>,<i>e</i>-C<sub>70</sub>O<sub>3</sub> when doped
with the heavy noble gas atoms Xe and Rn
Hybrid QM/QM Simulations of Excited-State Intramolecular Proton Transfer in the Molecular Crystal 7â(2-Pyridyl)-indole
A subtractive implementation of the QM/QM hybrid method
for the
description of photochemical reactions occurring in molecular crystals
is presented and tested by applying it in a simulation study of the
ultrafast intramolecular excited-state proton transfer reaction in
the crystal form of 7-(2-pyridyl)-indole, an organic compound featuring
an intramolecular hydrogen bond within a six-membered ring. By propagating
molecular dynamics on the excited-state potential energy surface,
a mean proton transfer time was calculated as 80 fs. The reaction
mechanism is discussed in terms of three-dimensional reaction coordinate
diagrams. Proton transfer was found to be barrierless and to be strongly
coupled to vibrational modes of the photoexcited molecule that modulate
the proton donorâacceptor distance. Some 300 fs after the initial
photoexcitation, the excited state molecule reached an S<sub>1</sub>/S<sub>0</sub> conical intersection through the mutual twist of the
pyridyl and indolyl moieties
Liquid Methanol from DFT and DFT/MM Molecular Dynamics Simulations
We present a comparative study of computational protocols
for the
description of liquid methanol from <i>ab initio</i> molecular
dynamics simulations, in view of further applications directed at
the modeling of chemical reactivity of organic and organometallic
molecules in (explicit) methanol solution. We tested density functional
theory molecular dynamics (DFT-MD) in its CarâParrinello Molecular
Dynamics (CPMD) and Quickstep/BornâOppenheimer MD (CP2K) implementations,
employing six popular density functionals with and without corrections
for dispersion interactions (namely BLYP, BLYP-D2, BLYP-D3, BP86,
BP86-D2, and B97-D2). Selected functionals were also tested within
the two QM/MM frameworks implemented in CPMD and CP2K, considering
one DFT molecule in a MM environment (described by the OPLS model
of methanol). The accuracy of each of these methods at describing
the bulk liquid phase under ambient conditions was evaluated by analyzing
their ability to reproduce (<i>i</i>) the average structure
of the liquid, (<i>ii</i>) the mean squared displacement
of methanol molecules, (<i>iii</i>) the average molecular
dipole moments, and (<i>iv</i>) the gas-to-liquid red-shift
observed in their infrared spectra. We show that it is difficult to
find a DFT functional that describes these four properties equally
well within full DFT-MD simulations, despite a good overall performance
of B97-D2. On the other hand, DFT/MM-MD provides a satisfactory description
of the solventâsolute polarization effects with all functionals
and thus represents a good alternative for the modeling of methanol
solutions in the context of chemical reactivity in an explicit environment
The Influence of the Hofmeister Bias and the Stability and Speciation of Chloridolanthanates on Their Extraction from Chloride Media
<p>The possibility of recovering rare earth elements from solutions containing their chloridometalate anions [LnCl<i><sub>x</sub></i>]<sup>(<i>x</i>â3)â</sup> via the process: LnCl<i><sub>x</sub></i><sup>(<i>x</i>â3)â</sup> + (<i>x</i> â 3)<i>L</i><sub>org</sub> + (<i>x</i>â3)H<sup>+</sup> â [(LH)<i><sub>x</sub></i><sub>â3</sub>LnCl<i><sub>x</sub></i>]<sub>org</sub> has been tested using 2-(1,3-bis(hexylamino)-1,3-dioxopropan-2-yl)-4,6-di-<i>tert</i>-butylpyridine (PMA), tri-<i>n-</i>butylphosphate (TBP), and tri-<i>n</i>-octylamine (TOA), which are known to be strong extractants for transition metal chloridometalates. While DFT calculations indicate that the formation of the neutral assembly [(PMAH)<sub>3</sub>LaCl<sub>6</sub>] in the gas phase is favorable, no uptake of La(III) from 6 M HCl by toluene solutions of PMA (or of TBP or TOA) was observed in solvent extraction experiments. Successful uptake of the [PtCl<sub>6</sub>]<sup>2â</sup> dianion by PMA and the failure to extract the [IrCl<sub>6</sub>]<sup>3â</sup> trianion under the same conditions indicate that the higher hydration energy of the latter makes transfer to the toluene solution less favorable and that this militates against extraction of La(III) chlorido complexes carrying charges of â3 or larger in which all the inner-sphere water molecules have been replaced. Computational results confirm literature observations that, in contrast to transition metal trications, formation of REE metalate anions such as [LnCl<i><sub>x</sub></i>]<sup>(<i>x</i>â3)â</sup> is not very favorable, particularly so for chloride, compared with nitrato or sulfato systems. Also, they indicate that the formation of <i>outer-sphere</i> assemblies such as {[La(H<sub>2</sub>O)<sub>9</sub>]·<i>x</i>Cl} in which water ligands are retained in the inner sphere, H-bonded to anions, is more stable than <i>inner-sphere</i> complexes containing an equivalent number of anions. The high level of hydration of such species disfavors their transfer into nonpolar water-immiscible solvents. It is unlikely that recovery of [LnCl<i><sub>x</sub></i>]<sup>(<i>x</i>â3)â</sup> from acidic solutions can be achieved efficiently using currently available anion exchange extractants operating in a âpH-swingâ process. Receptors giving very high binding energies to chloridolanthanates will be needed to offset the high dehydration energies required.</p
Elucidating the Breathing of the MetalâOrganic Framework MIL-53(Sc) with ab Initio Molecular Dynamics Simulations and in Situ Xâray Powder Diffraction Experiments
Ab initio molecular dynamics (AIMD)
simulations have been used
to predict structural transitions of the breathing metalâorganic
framework (MOF) MIL-53Â(Sc) in response to changes in temperature over
the range 100â623 K and adsorption of CO<sub>2</sub> at 0â0.9
bar at 196 K. The method has for the first time been shown to predict
successfully both temperature-dependent structural changes and the
structural response to variable sorbate uptake of a flexible MOF.
AIMD employing dispersion-corrected density functional theory accurately
simulated the experimentally observed closure of MIL-53Â(Sc) upon solvent
removal and the transition of the empty MOF from the <i>closed-pore</i> phase to the <i>very-narrow-pore</i> phase (symmetry change
from <i>P</i>2<sub>1</sub>/<i>c</i> to <i>C</i>2/<i>c</i>) with increasing temperature, indicating
that it can directly take into account entropic as well as enthalpic
effects. We also used AIMD simulations to mimic the CO<sub>2</sub> adsorption of MIL-53Â(Sc) in silico by allowing the MIL-53Â(Sc) framework
to evolve freely in response to CO<sub>2</sub> loadings corresponding
to the two steps in the experimental adsorption isotherm. The resulting
structures enabled the structure determination of the two CO<sub>2</sub>-containing <i>intermediate</i> and <i>large-pore</i> phases observed by experimental synchrotron X-ray diffraction studies
with increasing CO<sub>2</sub> pressure; this would not have been
possible for the <i>intermediate</i> structure via conventional
methods because of diffraction peak broadening. Furthermore, the strong
and anisotropic peak broadening observed for the <i>intermediate</i> structure could be explained in terms of fluctuations of the framework
predicted by the AIMD simulations. Fundamental insights from the molecular-level
interactions further revealed the origin of the breathing of MIL-53Â(Sc)
upon temperature variation and CO<sub>2</sub> adsorption. These simulations
illustrate the power of the AIMD method for the prediction and understanding
of the behavior of flexible microporous solids
Elucidating the Breathing of the MetalâOrganic Framework MIL-53(Sc) with ab Initio Molecular Dynamics Simulations and in Situ Xâray Powder Diffraction Experiments
Ab initio molecular dynamics (AIMD)
simulations have been used
to predict structural transitions of the breathing metalâorganic
framework (MOF) MIL-53Â(Sc) in response to changes in temperature over
the range 100â623 K and adsorption of CO<sub>2</sub> at 0â0.9
bar at 196 K. The method has for the first time been shown to predict
successfully both temperature-dependent structural changes and the
structural response to variable sorbate uptake of a flexible MOF.
AIMD employing dispersion-corrected density functional theory accurately
simulated the experimentally observed closure of MIL-53Â(Sc) upon solvent
removal and the transition of the empty MOF from the <i>closed-pore</i> phase to the <i>very-narrow-pore</i> phase (symmetry change
from <i>P</i>2<sub>1</sub>/<i>c</i> to <i>C</i>2/<i>c</i>) with increasing temperature, indicating
that it can directly take into account entropic as well as enthalpic
effects. We also used AIMD simulations to mimic the CO<sub>2</sub> adsorption of MIL-53Â(Sc) in silico by allowing the MIL-53Â(Sc) framework
to evolve freely in response to CO<sub>2</sub> loadings corresponding
to the two steps in the experimental adsorption isotherm. The resulting
structures enabled the structure determination of the two CO<sub>2</sub>-containing <i>intermediate</i> and <i>large-pore</i> phases observed by experimental synchrotron X-ray diffraction studies
with increasing CO<sub>2</sub> pressure; this would not have been
possible for the <i>intermediate</i> structure via conventional
methods because of diffraction peak broadening. Furthermore, the strong
and anisotropic peak broadening observed for the <i>intermediate</i> structure could be explained in terms of fluctuations of the framework
predicted by the AIMD simulations. Fundamental insights from the molecular-level
interactions further revealed the origin of the breathing of MIL-53Â(Sc)
upon temperature variation and CO<sub>2</sub> adsorption. These simulations
illustrate the power of the AIMD method for the prediction and understanding
of the behavior of flexible microporous solids
Inter- versus Intramolecular Structural Manipulation of a Dichromium(II) Pacman Complex through Pressure Variation
The
effect of pressure on the intranuclear M···M
separation and intermolecular secondary interactions in the dinuclear
chromium Pacman complex [Cr<sub>2</sub>(L)]Â(C<sub>6</sub>H<sub>6</sub>) was evaluated because this compound contains both a short Cr···Cr
separation and an exogenously bound molecule of benzene in the solid
state. The electronic structure of [Cr<sub>2</sub>(L)] was determined
by electron paramagnetic resonance spectroscopy, SQUID magnetometry,
and density functional theory calculations and shows a diamagnetic
ground state through antiferromagnetic exchange, with no evidence
for a CrâCr bond. Analysis of the solid-state structures of
[Cr<sub>2</sub>(L)]Â(C<sub>6</sub>H<sub>6</sub>) at pressures varying
from ambient to 3.0 GPa shows little deformation in the Cr···Cr
separation, i.e., no CrâCr bond formation, but instead a significantly
increased interaction between the exogenous arene and the chromium
iminopyrrolide environment. It is therefore apparent from this analysis
that [Cr<sub>2</sub>(L)] would be best exploited as a rigid chemical
synthon, with pressure regulation being used to mediate the approach
and secondary interactions of possible substrates
On the Extraction of HCl and H<sub>2</sub>PtCl<sub>6</sub> by Tributyl Phosphate: A Mode of Action Study
<p>Combining computational modeling with experimental measurements has revealed the self-assembly of nano-aggregate structures in the transfer of HCl and PtCl<sub>6</sub><sup>2â</sup> from an aqueous phase into toluene by the common industrial extractant tributyl phosphate (TBP). Molecular dynamics simulations have been coupled to analytical measurements to provide an atomistic interpretation of the mode of action of TBP under 6Â M and 10Â M HCl conditions. The structures conform to reverse micelles, where the Cl<sup>â</sup> or PtCl<sub>6</sub><sup>2â</sup> core is encapsulated by a hydration shell that acts as a mediating bridge to the electronegative oxygen atom in the TBP phosphate groups. For the 6Â M HCl extraction model, the data support stable aggregates forming from 2â3 TBP molecules around one chloride anion if the number of water molecules encapsulating the chloride anion is no more than five; increasing the water content to 10Â molecules allows a fourth TBP molecule to coordinate. For the 10Â M HCl extraction model, stable structures are obtained that conform to the empirical formula (TBP.HCl.H<sub>2</sub>O)<sub>3â5</sub>. At 6Â M HCl, extraction of PtCl<sub>6</sub><sup>2â</sup> is achieved by encapsulation by four TBP molecules; the data for extraction at 10Â M HCl indicate larger aggregates containing multiple PtCl<sub>6</sub><sup>2â</sup> anions are likely to be forming. In all cases, the hydrated core regions of the reverse micelles are considerably exposed. The diameters of the self-assembled structures around chloride ions agree well with available literature data from small-angle neutron-scattering experiments.</p
Experimental and DFTâD Studies of the Molecular Organic Energetic Material RDX
We have performed simulations utilizing
the dispersion-corrected
density functional theory method (DFT-D) as parametrized by Grimme
on selected polymorphs of RDX (cyclotrimethylenetrinitramine). Additionally,
we present the first experimental determination of the enthalpy of
fusion (Î<i>H</i><sub>fus</sub>) of the highly metastable
ÎČ-form of RDX. The characteristics of fusion for ÎČ-RDX
were determined to be 186.7 ± 0.8 °C, 188.5 ± 0.4 °C,
and 12.63 ± 0.28 kJ mol<sup>â1</sup> for the onset temperature,
peak temperature (or melting point), and Î<i>H</i><sub>fus</sub>, respectively. The difference in experimental Î<i>H</i><sub>fus</sub> for the α- and ÎČ-forms of RDX
is 20.46 ± 0.92 kJ mol<sup>â1</sup>. Ambient-pressure
lattice energies (<i>E</i><sub>L</sub>) of the α-
and ÎČ-forms of RDX have been calculated and are in excellent
agreement with experiment. In addition the computationally predicted
difference in <i>E</i><sub>L</sub> (20.35 kJ mol<sup>â1</sup>) between the α- and ÎČ-forms is in excellent agreement
with the experimental difference in Î<i>H</i><sub>fus</sub>. The response of the lattice parameters and unit-cell volumes
to pressure for the α- and γ-forms have been investigated,
in addition to the first high-pressure computational study of the
Δ-form of RDXîžthese results are in very good agreement
with experimental data. Phonon calculations provide good agreement
for vibrational frequencies obtained from Raman spectroscopy, and
a predicted inelastic neutron scattering (INS) spectrum of α-RDX
shows excellent agreement with experimental INS data determined in
this study. The transition energies and intensities are reproduced,
confirming that both the eigenvalues and the eigenvectors of the vibrations
are correctly described by the DFT-D method. The results of the high-pressure
phonon calculations have been used to show that the heat capacities
of the α-, γ-, and Δ-forms of RDX are only weakly
affected by pressure
Inter- versus Intramolecular Structural Manipulation of a Dichromium(II) Pacman Complex through Pressure Variation
The
effect of pressure on the intranuclear M···M
separation and intermolecular secondary interactions in the dinuclear
chromium Pacman complex [Cr<sub>2</sub>(L)]Â(C<sub>6</sub>H<sub>6</sub>) was evaluated because this compound contains both a short Cr···Cr
separation and an exogenously bound molecule of benzene in the solid
state. The electronic structure of [Cr<sub>2</sub>(L)] was determined
by electron paramagnetic resonance spectroscopy, SQUID magnetometry,
and density functional theory calculations and shows a diamagnetic
ground state through antiferromagnetic exchange, with no evidence
for a CrâCr bond. Analysis of the solid-state structures of
[Cr<sub>2</sub>(L)]Â(C<sub>6</sub>H<sub>6</sub>) at pressures varying
from ambient to 3.0 GPa shows little deformation in the Cr···Cr
separation, i.e., no CrâCr bond formation, but instead a significantly
increased interaction between the exogenous arene and the chromium
iminopyrrolide environment. It is therefore apparent from this analysis
that [Cr<sub>2</sub>(L)] would be best exploited as a rigid chemical
synthon, with pressure regulation being used to mediate the approach
and secondary interactions of possible substrates