13 research outputs found
Molecular Dynamics Simulations of Alkylsilane Monolayers on Silica Nanoasperities: Impact of Surface Curvature on Monolayer Structure and Pathways for Energy Dissipation in Tribological Contacts
Self-assembled monolayers (SAMs) of alkylsilanes have
been considered
as wear reducing layers in tribological applications, particularly
to reduce stiction and wear in microelectromechanical systems (MEMS)
devices. Though these films successfully reduce interfacial forces,
they are easily damaged during impact and shear. Surface roughness
at the nanoscale is believed to play an important role in the failure
of these films because it effects both the formation and quality of
SAMs, and it focuses interfacial contact forces to very small areas,
magnifying the locally applied pressure and shear on the lubricant
film. To complement our prior studies employing Fourier transform
infrared spectroscopy (FTIR) and atomic force microscopy (AFM) experiments
in which silica nanoparticles are used to simulate nanoasperities
and to refine our analysis of these films to a molecular level, classical
molecular dynamics simulations have been employed to understand the
impact of nanoscopic surface curvature on the properties of alkylsilane
SAMs. Amorphous silica nanoparticles of various radii were prepared
to simulate single asperities on a rough MEMS device surface, or AFM
tips, which were then functionalized with alkylsilane SAMs of varying
chain lengths. Factors related to the tribological performance of
the film, including <i>gauche</i> defect density and exposed
silica surface area, were examined to understand the impact of surface
curvature on the film. Additionally, because the packing density of
the films has been found to be relatively low for alkylsilane SAMs
on surfaces with nanoscopic curvature, packing density studies were
performed on simulated silica surfaces lacking curvature to understand
the relative impact of these two important factors. It was found that
both curvature and packing density affect the film quality; however,
packing density was found to have the strongest correlation to film
quality, demonstrating that greater priority should be given to the
reduction of free volume within the films to improve their structural
rigidity, to better passivate the underlying surfaces of the devices,
and to improve the extent and accessibility of nondestructive dissipation
pathways, all of which will lead to improved friction and wear resistance.
While focused on silica nanoasperities, these MD simulations afford
general approaches for studies of ligand effects on a range of surfaces
with nanoscopic curvature such as metal oxide nanoparticles and quantum
dots
Molecular Dynamics Simulations of Alkylsilane Monolayers on Silica Nanoasperities: Impact of Surface Curvature on Monolayer Structure and Pathways for Energy Dissipation in Tribological Contacts
Self-assembled monolayers (SAMs) of alkylsilanes have
been considered
as wear reducing layers in tribological applications, particularly
to reduce stiction and wear in microelectromechanical systems (MEMS)
devices. Though these films successfully reduce interfacial forces,
they are easily damaged during impact and shear. Surface roughness
at the nanoscale is believed to play an important role in the failure
of these films because it effects both the formation and quality of
SAMs, and it focuses interfacial contact forces to very small areas,
magnifying the locally applied pressure and shear on the lubricant
film. To complement our prior studies employing Fourier transform
infrared spectroscopy (FTIR) and atomic force microscopy (AFM) experiments
in which silica nanoparticles are used to simulate nanoasperities
and to refine our analysis of these films to a molecular level, classical
molecular dynamics simulations have been employed to understand the
impact of nanoscopic surface curvature on the properties of alkylsilane
SAMs. Amorphous silica nanoparticles of various radii were prepared
to simulate single asperities on a rough MEMS device surface, or AFM
tips, which were then functionalized with alkylsilane SAMs of varying
chain lengths. Factors related to the tribological performance of
the film, including <i>gauche</i> defect density and exposed
silica surface area, were examined to understand the impact of surface
curvature on the film. Additionally, because the packing density of
the films has been found to be relatively low for alkylsilane SAMs
on surfaces with nanoscopic curvature, packing density studies were
performed on simulated silica surfaces lacking curvature to understand
the relative impact of these two important factors. It was found that
both curvature and packing density affect the film quality; however,
packing density was found to have the strongest correlation to film
quality, demonstrating that greater priority should be given to the
reduction of free volume within the films to improve their structural
rigidity, to better passivate the underlying surfaces of the devices,
and to improve the extent and accessibility of nondestructive dissipation
pathways, all of which will lead to improved friction and wear resistance.
While focused on silica nanoasperities, these MD simulations afford
general approaches for studies of ligand effects on a range of surfaces
with nanoscopic curvature such as metal oxide nanoparticles and quantum
dots
Driving Surface Chemistry at the Nanometer Scale Using Localized Heat and Stress
Driving and measuring chemical reactions at the nanoscale is crucial
for developing safer, more efficient, and environment-friendly reactors
and for surface engineering. Quantitative understanding of surface
chemical reactions in real operating environments is challenging due
to resolution and environmental limitations of existing techniques.
Here we report an atomic force microscope technique that can measure
reaction kinetics driven at the nanoscale by multiphysical stimuli
in an ambient environment. We demonstrate the technique by measuring
local reduction of graphene oxide as a function of both temperature
and force at the sliding contact. Kinetic parameters measured with
this technique reveal alternative reaction pathways of graphene oxide
reduction previously unexplored with bulk processing techniques. This
technique can be extended to understand and precisely tailor the nanoscale
surface chemistry of any two-dimensional material in response to a
wide range of external, multiphysical stimuli
Surface Curvature Enhances the Electrotunability of Ionic Liquid Lubrication
Ionic liquids (ILs) are a promising class of lubricants
that allow
dynamic friction control at electrified interfaces. In the real world,
surfaces inevitably exhibit some degree of roughness, which can influence
lubrication. In this work, we deposited single-layer graphene onto
20 nm silica nanoparticle films to investigate the effect of surface
curvature and electrostatic potential on both the lubricious behavior
and interfacial layering structure of 1-ethyl-3-methyl imidazolium
bis(trifluoromethylsulfonyl)imide on graphene. Normal force and friction
force measurements were conducted by atomic force microscopy using
a sharp silicon tip. Our results reveal that the friction coefficient
at the lubricated tip–graphene contacts significantly depends
on surface curvature. Two friction coefficients are measured on graphene
peaks and valleys with a higher coefficient measured at lower loads
(pressures), whereas only one friction coefficient is measured on
smooth graphene. Moreover, the electrotunability of the friction coefficient
at low loads is observed to be significantly enhanced in peaks and
valleys compared with smooth graphene. This is associated with the
promoted overscreening of surface charge on convex interfaces and
the steric hindrance at concave interfaces, which leads to more layers
of ions (electrostatically) bound to the surface, i.e., thicker boundary
films (electrical double layers). This work opens new avenues to control
IL lubrication on the nanoscale by combining topographic features
and an electric field
Robust and Flexible Aramid Nanofiber/Graphene Layer-by-Layer Electrodes
Aramid
nanofibers (ANFs), or nanoscale Kevlar fibers, are of interest for
their high mechanical performance and functional nanostructure. The
dispersible nature of ANFs opens up processing opportunities for creating
mechanically robust and flexible nanocomposites, particularly for
energy and power applications. The challenge is to manipulate ANFs
into an electrode structure that balances mechanical and electrochemical
performance to yield a robust and flexible electrode. Here, ANFs and
graphene oxide (GO) sheets are blended using layer-by-layer (LbL)
assembly to achieve mechanically flexible supercapacitor electrodes.
After reduction, the resulting electrodes exhibit an ANF-rich structure
where ANFs act as a polymer matrix that interfacially interacts with
reduced graphene oxide sheets. It is shown that ANF/GO deposition
proceeds by hydrogen bonding and π–π interactions,
leading to linear growth (1.2 nm/layer pairs) and a composition of
75 wt % ANFs and 25 wt % GO sheets. Chemical reduction leads to a
high areal capacitance of 221 μF/cm<sup>2</sup>, corresponding
to 78 F/cm<sup>3</sup>. Nanomechanical testing shows that the electrodes
have a modulus intermediate between those of the two native materials.
No cracks or defects are observed upon flexing ANF/GO films 1000 times
at a radius of 5 mm, whereas a GO control shows extensive cracking.
These results demonstrate that electrodes containing ANFs and reduced
GO sheets are promising for flexible, mechanically robust energy and
power
Effects of Direct Solvent-Quantum Dot Interaction on the Optical Properties of Colloidal Monolayer WS<sub>2</sub> Quantum Dots
Because of the absence
of native dangling bonds on the surface
of the layered transition metal dichalcogenides (TMDCs), the surface
of colloidal quantum dots (QDs) of TMDCs is exposed directly to the
solvent environment. Therefore, the optical and electronic properties
of TMDCS QDs are expected to have stronger influence from the solvent
than usual surface-passivated QDs due to more direct solvent-QD interaction.
Study of such solvent effect has been difficult in colloidal QDs of
TMDC due to the large spectroscopic heterogeneity resulting from the
heterogeneity of the lateral size or (and) thickness in ensemble.
Here, we developed a new synthesis procedure producing the highly
uniform colloidal monolayer WS<sub>2</sub> QDs exhibiting well-defined
photoluminescence (PL) spectrum free from ensemble heterogeneity.
Using these newly synthesized monolayer WS<sub>2</sub> QDs, we observed
the strong influence of the aromatic solvents on the PL energy and
intensity of monolayer WS<sub>2</sub> QD beyond the simple dielectric
screening effect, which is considered to result from the direct electronic
interaction between the valence band of the QDs and molecular orbital
of the solvent. We also observed the large effect of stacking/separation
equilibrium on the PL spectrum dictated by the balance between inter
QD and QD-solvent interactions. The new capability to probe the effect
of the solvent molecules on the optical properties of colloidal TMDC
QDs will be valuable for their applications in various liquid surrounding
environments
Using Particle Lithography to Tailor the Architecture of Au Nanoparticle Plasmonic Nanoring Arrays
The
facile assembly of metal nanostructured arrays is a fundamental
step in the design of plasmon enhanced chemical sensing and solar
cell architectures. Here we have investigated methods of creating
controlled formations of two-dimensional periodic arrays comprised
of 20 nm Au nanoparticles (NPs) on a hydrophilic polymer surface using
particle lithography. To direct the assembly process, capillary force
and NP concentration both play critical roles on the resulting nanostructured
arrays. As such, tuning these experimental parameters can directly
be used to modify the nature of the nanostructures formed. To explore
this, two different concentrations of Au NP solutions (∼7 ×
10<sup>11</sup> or 4 × 10<sup>12</sup> NPs/mL) were used in conjunction
with a fixed concentration of polystyrene microspheres (PS MS, ∼6
× 10<sup>9</sup> PS MS/mL). Assembly at a relative humidity (RH)
of 45% with the higher concentration resulted in the formation of
well-defined Au nanorings of ca. 23 nm in height and 881 nm in diameter
with a pitch of 2.5 μm. Assembly at 65% RH with the lower concentration
of NPs resulted in Au nanodonut arrays comprised of isolated single
Au NPs. To explore the extent of coupling in the well-defined structures,
dark field scattering spectra were collected and showed a broad localized
surface plasmon resonance (LSPR) peak with a shoulder, which full-wave
electrodynamics modeling (finite-difference time domain (FDTD) method)
attributed to be a result of pronounced particle–particle coupling
along the circumference of the nanoring array
Reversible Changes in Solution pH Resulting from Changes in Thermoresponsive Polymer Solubility
Pendant groups on polymers that have lower-critical solution
temperature (LCST) properties experience a water-like environment
below the LCST where the polymer is soluble but are less hydrated
above the LCST when the polymer phase separates from solution. When
these pendant groups are amphoteric groups like carboxylate salts
or ammonium salts, the change in solvation that accompanies the polymer
precipitation event significantly changes these groups’ acidity
or basicity. These changes in acidity or basicity can lead to carboxylate
salts forming carboxylic acid groups by capturing protons from the
bulk solvent or ammonium salts reverting to the neutral amine by release
of protons to the bulk solvent, respectively. When polymers like polyÂ(<i>N</i>-isopropylacrylamide) that contain a sufficient loading
of such comonomers are dissolved in solutions whose pH is near the
p<i>K</i><sub>a</sub> of the pendant acid or basic group
and undergo
an LCST event, the LCST event can change the bulk solution pH. These
changes are reversible. These effects were visually followed using
common indicators with soluble polymers and or by monitoring solution
pH as a function of temperature. LCST events triggered by the addition
of a kosmotropic salt lead to similar reversible solution pH changes
Fabrication and Electrochemical Performance of Structured Mesoscale Open Shell V<sub>2</sub>O<sub>5</sub> Networks
Crystalline vanadium
pentoxide (V<sub>2</sub>O<sub>5</sub>) has
attracted significant interest as a potential cathode material for
energy storage applications due to its high theoretical capacity.
Unfortunately, the material suffers from low conductivity as well
as slow lithium ion diffusion, both of which affect how fast the electrode
can be charged/discharged and how many times it can be cycled. Colloidal
crystal templating (CCT) provides a simple approach to create well-organized
3-D nanostructures of materials, resulting in a significant increase
in surface area that can lead to marked improvements in electrochemical
performance. Here, a single layer of open shell V<sub>2</sub>O<sub>5</sub> architectures ca. 1 μm in height with ca. 100 nm wall
thickness was fabricated using CCT, and the electrochemical properties
of these assemblies were evaluated. A decrease in polarization effects,
resulting from the higher surface area mesostructured features, was
found to produce significantly enhanced electrochemical performance.
The discharge capacity of an unpatterned thin film of V<sub>2</sub>O<sub>5</sub> (∼8.1 μAh/cm<sup>2</sup>) was found to
increase to ∼10.2 μAh/cm<sup>2</sup> when the material
was patterned by CCT, affording enhanced charge storage capabilities
as well as a decrease in the irreversible degradation during charge–discharge
cycling. This work demonstrates the importance of creating mesoscale
electrode surfaces for improving the performance of energy storage
devices and provides fundamental understanding of the means to improve
device performance
Reversible Changes in Solution pH Resulting from Changes in Thermoresponsive Polymer Solubility
Pendant groups on polymers that have lower-critical solution
temperature (LCST) properties experience a water-like environment
below the LCST where the polymer is soluble but are less hydrated
above the LCST when the polymer phase separates from solution. When
these pendant groups are amphoteric groups like carboxylate salts
or ammonium salts, the change in solvation that accompanies the polymer
precipitation event significantly changes these groups’ acidity
or basicity. These changes in acidity or basicity can lead to carboxylate
salts forming carboxylic acid groups by capturing protons from the
bulk solvent or ammonium salts reverting to the neutral amine by release
of protons to the bulk solvent, respectively. When polymers like polyÂ(<i>N</i>-isopropylacrylamide) that contain a sufficient loading
of such comonomers are dissolved in solutions whose pH is near the
p<i>K</i><sub>a</sub> of the pendant acid or basic group
and undergo
an LCST event, the LCST event can change the bulk solution pH. These
changes are reversible. These effects were visually followed using
common indicators with soluble polymers and or by monitoring solution
pH as a function of temperature. LCST events triggered by the addition
of a kosmotropic salt lead to similar reversible solution pH changes