10 research outputs found
Fundamentals of Crystalline Evolution and Properties of Carbon Nanotube-Reinforced Polyether Ether Ketone Nanocomposites in Fused Filament Fabrication
As fused filament fabrication (FFF) continues to gain
popularity,
many studies are turning to nanomaterials or optimization of printing
parameters to improve the materialsā properties; however, many
overlook how materials formulation and additive manufacturing (AM)
processes cooperatively engineer the evolution of properties across
length scales. Evaluating the in-process evolution of the nanocomposite
using AM will provide a fundamental understanding of the materialās
microstructure, which can be tailored to create unique characteristics
in functionality and performance. In this study, the crystallinity
behavior of polyetheretherketone (PEEK) was studied in the presence
of carbon nanotubes (CNTs) as a nucleation aid for improved crystallization
during FFF processing. Using various characterization techniques and
molecular dynamics simulations, it was discovered that the crystallization
behavior of extruded filaments is very different from that of 3D printed
roads. Additionally, the printed material exhibited cold crystallization,
and the CNT addition increased the crystallization of printed roads,
which were amorphous without CNT addition. Tensile strength and modulus
were increased by as much as 42 and 51%, respectively, due to higher
crystallinity during printing. Detailed knowledge on the morphology
of PEEKāCNT used in FFF allows gaining a fundamental understanding
of the morphological evolution occurring during the AM process that
in turn enables formulating materials for the AM process to achieve
tailored mechanical and functional properties, such as crystallinity
or conductivity
Mechanistic Investigations of the ZnCl<sub>2</sub>-Mediated Tandem Mukaiyama Aldol Lactonization: Evidence for Asynchronous, Concerted Transition States and Discovery of 2-Oxopyridyl Ketene Acetal Variants
The ZnCl<sub>2</sub>-mediated tandem Mukaiyama aldol
lactonization
(TMAL) reaction of aldehydes and thiopyridyl ketene acetals provides
a versatile, highly diastereoselective approach to <i>trans</i>-1,2-disubstituted Ī²-lactones. Mechanistic and theoretical
studies described herein demonstrate that both the efficiency of this
process and the high diastereoselectivity are highly dependent upon
the type of ketene acetal employed but independent of ketene acetal
geometry. Significantly, we propose a novel and distinct mechanistic
pathway for the ZnCl<sub>2</sub>-mediated TMAL process versus other
Mukaiyama aldol reactions based on our experimental evidence to date
and further supported by calculations (B3LYP/BSI). Contrary to the
commonly invoked mechanistic extremes of [2+2] cycloaddition and aldol
lactonization mechanisms, investigations of the TMAL process suggest
a concerted but asynchronous transition state between aldehydes and
thiopyridyl ketene acetals. These calculations support a boat-like
transition state that differs from commonly invoked Mukaiyama āopenā
or ZimmermanāTraxler āchair-likeā transition-state
models. Furthermore, experimental studies support the beneficial effect
of pre-coordination between ZnCl<sub>2</sub> and thiopyridyl ketene
acetals prior to aldehyde addition for optimal reaction rates. Our
previously proposed, silylated Ī²-lactone intermediate that led
to successful TMAL-based cascade sequences is also supported by the
described calculations and ancillary experiments. These findings suggested
that a similar TMAL process leading to Ī²-lactones would be possible
with an oxopyridyl ketene acetal, and this was confirmed experimentally,
leading to a novel TMAL process that proceeds with efficiency comparable
to that of the thiopyridyl system
Studies of Ligand Exchange in N-Heterocyclic Carbene Silver(I) Complexes
A series of N-heterocyclic carbene (NHC) AgĀ(I) complexes
have been
prepared and used to study the dynamics of NHC ligand exchange in
these AgĀ(I) complexes. These studies used solution-state variable-temperature
(VT) <sup>13</sup>C NMR spectroscopy and the temperature-dependent
changes in <sup>13</sup>Cā<sup>107/109</sup>Ag coupling to
determine activation energies for the ligand exchange process. The
effects of concentration, bridging anions, and additives on the exchange
process have been studied. The experimental activation energies for
the NHC ligand exchange processes of these silver complexes are also
compared with DFT calculations. The results are consistent with an
associative mechanism for the AgĀ(I)āNHC exchange process
Studies of Ligand Exchange in N-Heterocyclic Carbene Silver(I) Complexes
A series of N-heterocyclic carbene (NHC) AgĀ(I) complexes
have been
prepared and used to study the dynamics of NHC ligand exchange in
these AgĀ(I) complexes. These studies used solution-state variable-temperature
(VT) <sup>13</sup>C NMR spectroscopy and the temperature-dependent
changes in <sup>13</sup>Cā<sup>107/109</sup>Ag coupling to
determine activation energies for the ligand exchange process. The
effects of concentration, bridging anions, and additives on the exchange
process have been studied. The experimental activation energies for
the NHC ligand exchange processes of these silver complexes are also
compared with DFT calculations. The results are consistent with an
associative mechanism for the AgĀ(I)āNHC exchange process
Computational Insights into Uranium Complexes Supported by Redox-Active Ī±-Diimine Ligands
The electronic structures of two uranium compounds supported
by
redox-active Ī±-diimine ligands, (<sup>Mes</sup>DAB<sup>Me</sup>)<sub>2</sub>UĀ(THF) (<b>1</b>) and Cp<sub>2</sub>UĀ(<sup>Mes</sup>DAB<sup>Me</sup>) (<b>2</b>) (<sup>Mes</sup>DAB<sup>Me</sup> = [ArNī»CĀ(Me)ĀCĀ(Me)ī»NAr]; Ar = 2,4,6-trimethylphenyl
(Mes)), have been investigated using both density functional theory
and multiconfigurational self-consistent field methods. Results from
these studies have established that both uranium centers are tetravalent,
that the ligands are reduced by two electrons, and that the ground
states of these molecules are triplets. Energetically low-lying singlet
states are accessible, and some transitions to these states are visible
in the electronic absorption spectrum
Computational Insights into Uranium Complexes Supported by Redox-Active Ī±-Diimine Ligands
The electronic structures of two uranium compounds supported
by
redox-active Ī±-diimine ligands, (<sup>Mes</sup>DAB<sup>Me</sup>)<sub>2</sub>UĀ(THF) (<b>1</b>) and Cp<sub>2</sub>UĀ(<sup>Mes</sup>DAB<sup>Me</sup>) (<b>2</b>) (<sup>Mes</sup>DAB<sup>Me</sup> = [ArNī»CĀ(Me)ĀCĀ(Me)ī»NAr]; Ar = 2,4,6-trimethylphenyl
(Mes)), have been investigated using both density functional theory
and multiconfigurational self-consistent field methods. Results from
these studies have established that both uranium centers are tetravalent,
that the ligands are reduced by two electrons, and that the ground
states of these molecules are triplets. Energetically low-lying singlet
states are accessible, and some transitions to these states are visible
in the electronic absorption spectrum
Utilizing Nearest-Neighbor Interactions To Alter Charge Transport Mechanisms in Molecular Assemblies of Porphyrins on Surfaces
When
tunneling is the dominant mechanism of charge transport in
a molecular junction, the conductivity of the junction is largely
insensitive to chemical and structural perturbations which do not
impact the overall length of the junction. This severely hampers the
seemingly limitless potential of molecules to modulate charge transport
at interfaces and their application in a host of device designs. This
is a particular challenge for molecules baring insulating features
like saturated hydrocarbons which decouple functional groups from
the surface. Such decoupling groups increase the energy required to
isolate charge on the molecule, pushing transport into the tunneling
regime in many cases. Herein, we demonstrate that, through enhancement
of nearest neighbor interactions, lateral delocalization of charge
states in molecular islands can be used to shift transport out of
the tunneling regime to the more efficient, and more chemically tunable,
charge-hopping regime. In a previous study, it was found that through-bond
tunneling was the dominant mechanism of charge transport through a
hydrocarbon-tethered free-base porphyrin thiol. With coordination
of zincĀ(II), the formation of large molecular islands in an alkanethiol
matrix on a Au(111) surface was facilitated. Bias-induced switching
and unphysical tunneling efficiencies observed by scanning tunneling
microscopy of these molecular islands, as well as Coulomb blockade
observed in low-temperature crossed-wire tunnel junction measurements,
indicate charge hopping becomes the dominant mechanism of transport
in the molecular islands, whereas transport in single molecules was
consistent with through-bond tunneling. These results elucidate the
basis for functional conductivityāstructure and supramolecular
relationships that may be employed in the design of molecular junctions
in organic thin films
Computational Insights into Uranium Complexes Supported by Redox-Active Ī±-Diimine Ligands
The electronic structures of two uranium compounds supported
by
redox-active Ī±-diimine ligands, (<sup>Mes</sup>DAB<sup>Me</sup>)<sub>2</sub>UĀ(THF) (<b>1</b>) and Cp<sub>2</sub>UĀ(<sup>Mes</sup>DAB<sup>Me</sup>) (<b>2</b>) (<sup>Mes</sup>DAB<sup>Me</sup> = [ArNī»CĀ(Me)ĀCĀ(Me)ī»NAr]; Ar = 2,4,6-trimethylphenyl
(Mes)), have been investigated using both density functional theory
and multiconfigurational self-consistent field methods. Results from
these studies have established that both uranium centers are tetravalent,
that the ligands are reduced by two electrons, and that the ground
states of these molecules are triplets. Energetically low-lying singlet
states are accessible, and some transitions to these states are visible
in the electronic absorption spectrum
Diruthenium Naphthalene and Anthracene Complexes Containing a Doubly Linked Dicyclopentadienyl Ligand
The reaction of <i>cis</i>-{(Ī·<sup>5</sup>-C<sub>5</sub>H<sub>3</sub>)<sub>2</sub>(CMe<sub>2</sub>)<sub>2</sub>}ĀRu<sub>2</sub>(CO)<sub>4</sub>Br<sub>2</sub> with naphthalene affords
the <i>syn</i>-facial [<i>cis</i>-{(Ī·<sup>5</sup>-C<sub>5</sub>H<sub>3</sub>)<sub>2</sub>(CMe<sub>2</sub>)<sub>2</sub>}ĀRu<sub>2</sub>(Ī¼-Ī·<sup>6</sup>,Ī·<sup>6</sup>-C<sub>10</sub>H<sub>8</sub>)]Ā[OTf]<sub>2</sub>, (<b>2</b><sup><b>2+</b></sup>), a complex that appears to be two electrons
short of the
18-electron rule. Density functional theory (DFT) calculations suggest
that the Ru atoms satisfy their missing valence by a combination of
a weak metalāmetal bond and sharing electrons from the central
Ļ bond of the naphthalene. The one-electron reduction of <b>2</b><sup><b>2+</b></sup> yields <b>2</b><sup><b>+</b></sup>, a Class II mixed-valence complex, while the two-electron
reduction of <b>2</b><sup><b>2+</b></sup> causes a hapticity
change from Ī·<sup>6</sup> to Ī·<sup>4</sup> on one of the
naphthalene rings and yields <i>cis</i>-{(Ī·<sup>5</sup>-C<sub>5</sub>H<sub>3</sub>)<sub>2</sub>(CMe<sub>2</sub>)<sub>2</sub>}ĀRu<sub>2</sub>(Ī¼-Ī·<sup>6</sup>,Ī·<sup>4</sup>-C<sub>10</sub>H<sub>8</sub><b>)</b> (<b>2</b><sup><b>0</b></sup>), a zwitterionic complex. The DFT calculations predict that
the <i>C</i><sub><i>s</i></sub> isomer of <b>2<sup>0</sup></b> is 4.69 kcal/mol lower in energy than the <i>C</i><sub>2<i>v</i></sub> isomer, which is a transition
state. Reaction of <i>cis</i>-{(Ī·<sup>5</sup>-C<sub>5</sub>H<sub>3</sub>)<sub>2</sub>(CMe<sub>2</sub>)<sub>2</sub>}ĀRu<sub>2</sub>(CO)<sub>4</sub>Br<sub>2</sub> with anthracene affords the
analogous <i>syn</i>-facial anthracene complex, [<i>cis</i>-{(Ī·<sup>5</sup>-C<sub>5</sub>H<sub>3</sub>)<sub>2</sub>(CMe<sub>2</sub>)<sub>2</sub>}ĀRu<sub>2</sub>(Ī¼-Ī·<sup>6</sup>,Ī·<sup>6</sup>-C<sub>14</sub>H<sub>10</sub>)]Ā[OTf]<sub>2</sub>, (<b>4</b>), and the tetranuclear dianthracene complex,
[<i>cis</i>-{(Ī·<sup>5</sup>-C<sub>5</sub>H<sub>3</sub>)<sub>2</sub>(CMe<sub>2</sub>)<sub>2</sub>}ĀRu<sub>2</sub>(Ī¼-Ī·<sup>6</sup>,Ī·<sup>6</sup>-C<sub>14</sub>H<sub>10</sub>)]<sub>2</sub>[OTf]<sub>4</sub>, (<b>5</b>). <b>2</b><sup><b>2+</b></sup>, <b>2</b><sup><b>0</b></sup>, and <b>5</b> were structurally characterized by X-ray diffraction
Diruthenium Naphthalene and Anthracene Complexes Containing a Doubly Linked Dicyclopentadienyl Ligand
The reaction of <i>cis</i>-{(Ī·<sup>5</sup>-C<sub>5</sub>H<sub>3</sub>)<sub>2</sub>(CMe<sub>2</sub>)<sub>2</sub>}ĀRu<sub>2</sub>(CO)<sub>4</sub>Br<sub>2</sub> with naphthalene affords
the <i>syn</i>-facial [<i>cis</i>-{(Ī·<sup>5</sup>-C<sub>5</sub>H<sub>3</sub>)<sub>2</sub>(CMe<sub>2</sub>)<sub>2</sub>}ĀRu<sub>2</sub>(Ī¼-Ī·<sup>6</sup>,Ī·<sup>6</sup>-C<sub>10</sub>H<sub>8</sub>)]Ā[OTf]<sub>2</sub>, (<b>2</b><sup><b>2+</b></sup>), a complex that appears to be two electrons
short of the
18-electron rule. Density functional theory (DFT) calculations suggest
that the Ru atoms satisfy their missing valence by a combination of
a weak metalāmetal bond and sharing electrons from the central
Ļ bond of the naphthalene. The one-electron reduction of <b>2</b><sup><b>2+</b></sup> yields <b>2</b><sup><b>+</b></sup>, a Class II mixed-valence complex, while the two-electron
reduction of <b>2</b><sup><b>2+</b></sup> causes a hapticity
change from Ī·<sup>6</sup> to Ī·<sup>4</sup> on one of the
naphthalene rings and yields <i>cis</i>-{(Ī·<sup>5</sup>-C<sub>5</sub>H<sub>3</sub>)<sub>2</sub>(CMe<sub>2</sub>)<sub>2</sub>}ĀRu<sub>2</sub>(Ī¼-Ī·<sup>6</sup>,Ī·<sup>4</sup>-C<sub>10</sub>H<sub>8</sub><b>)</b> (<b>2</b><sup><b>0</b></sup>), a zwitterionic complex. The DFT calculations predict that
the <i>C</i><sub><i>s</i></sub> isomer of <b>2<sup>0</sup></b> is 4.69 kcal/mol lower in energy than the <i>C</i><sub>2<i>v</i></sub> isomer, which is a transition
state. Reaction of <i>cis</i>-{(Ī·<sup>5</sup>-C<sub>5</sub>H<sub>3</sub>)<sub>2</sub>(CMe<sub>2</sub>)<sub>2</sub>}ĀRu<sub>2</sub>(CO)<sub>4</sub>Br<sub>2</sub> with anthracene affords the
analogous <i>syn</i>-facial anthracene complex, [<i>cis</i>-{(Ī·<sup>5</sup>-C<sub>5</sub>H<sub>3</sub>)<sub>2</sub>(CMe<sub>2</sub>)<sub>2</sub>}ĀRu<sub>2</sub>(Ī¼-Ī·<sup>6</sup>,Ī·<sup>6</sup>-C<sub>14</sub>H<sub>10</sub>)]Ā[OTf]<sub>2</sub>, (<b>4</b>), and the tetranuclear dianthracene complex,
[<i>cis</i>-{(Ī·<sup>5</sup>-C<sub>5</sub>H<sub>3</sub>)<sub>2</sub>(CMe<sub>2</sub>)<sub>2</sub>}ĀRu<sub>2</sub>(Ī¼-Ī·<sup>6</sup>,Ī·<sup>6</sup>-C<sub>14</sub>H<sub>10</sub>)]<sub>2</sub>[OTf]<sub>4</sub>, (<b>5</b>). <b>2</b><sup><b>2+</b></sup>, <b>2</b><sup><b>0</b></sup>, and <b>5</b> were structurally characterized by X-ray diffraction