14 research outputs found
Manipulation of Polymer/Polymer Interface Width from Nonequilibrium Deposition
We demonstrate, using neutron reflectivity,
that the width of a
nonequilibrium interface between an organo-soluble aromatic polyimide
film and triacetate cellulose (TAC) support film created by spin-coating
or solution-casting can be broadened in a controllable way using a
âswelling agentâ in the deposition process. In a favorable
case, the adhesion, as measured by T-peel tests, can be increased
by a factor of 7 by adjustment of the solvent composition. The morphologies
of the TAC fractured surfaces after peeling tests measured by AFM
reveal that broadening of the interfacial width causes an interconnected
network in the interface, leading to a sharp increase in the interfacial
adhesion. Differences in the chemistry (solubility) of the materials
being deposited do make a difference in the effectiveness of this
strategy of using a âswelling agentâ. For one polyimide,
a 3-fold increase in adhesion can be obtained by optimizing the deposition
temperature, but this approach for improving adhesion is less effective
than that of adding âswelling agentâ. The formation
of robust interfaces of this type is important because of the critical
roles that multilayer films containing polymers with special properties
and tailored structures play in applications as diverse as computer
displays, photovoltaic devices, and polymeric electronics. The âswelling
agentâ strategy makes it possible to produce polymer multilayer
structures in a cost-effective way with roll-to-roll mass production
using direct solution coating
Molecular Weight Dependence on the Disintegration of Spin-Assisted Weak Polyelectrolyte Multilayer Films
We present the effect of molecular
weight (MW) of polyelectrolytes (PEs) on the disintegration behavior
of weak PE multilayer films consisting of linear polyÂ(ethylene imine)
(LPEI) and polyÂ(methacrylic acid) (PMAA). The multilayer films prepared
by the spin-assisted layer-by-layer deposition have well-ordered internal
structures and also show the linear thickness growth behavior regardless
of MWs of PMAA. The well-defined weak PE multilayer films were subject
to disintegration into bulk solution when the electrostatic interactions
between LPEI and PMAA layers were reduced by treatment at pH 2. However,
we demonstrated the change in the disintegration mode and kinetics
(i.e., from burst erosion to controlled surface erosion) as a function
of MW of PMAA based on neutron reflectivity and quartz crystal microbalance
with dissipation, revealing the correlation between the structural
changes and the viscoelastic responses of the weak PE films upon pH
treatment. Also, the unique swelling behavior as well as the significant
increase in dissipation energy was monitored before the complete disintegration
of the multilayer films containing high MW PMAA, which is believed
to originate from their slow rearrangement kinetics within the film.
We believe that the results shown in this study provide chain-level
understanding as to the MW-dependence on pH-triggered disintegration
mechanism of weak PE multilayer films
Controlled Release from Model Blend Multilayer Films Containing Mixtures of Strong and Weak Polyelectrolytes
We have designed the controlled release platforms based
on polyelectrolyte
(PE) blend multilayer films to investigate the release mode and kinetics
at the nanoscale level. The model blend multilayer films are composed
of positively charged layers with weak polyelectrolytes (PEs) (linear
polyÂ(ethylenimine), LPEI) and negatively charged blend layers with
mixtures of strong (polyÂ(sodium 4-styrenesulfonic acid), PSS) and
weak (polyÂ(methacrylic acid), PMAA) PEs. The blend multilayer films
([LPEI/PSS:PMAA]<sub><i>n</i></sub>) with well-defined internal
structure were prepared by the spin-assisted layer-by-layer (LbL)
deposition method. Release properties of the multilayer films were
systematically studied as a function of blend ratio by neutron reflectivity
(NR), ellipsometer, AFM, FT-IR spectroscopy, and quartz crystal microbalance
with dissipation (QCM-D). Since PSS strong PEs serve as robust skeletons
within the multilayer films independent of external pH variation,
the burst disruption of pure weak PE multilayer films was dramatically
suppressed, and the release kinetics could be accurately controlled
by simply changing the PSS content within the blend films. These release
properties of blend multilayer films form the basis for designing
the controlled release of target active materials from surfaces
Scaling Behavior and Segment Concentration Profile of Densely Grafted Polymer Brushes Swollen in Vapor
The
scaling of the thickness, <i>h</i><sub>s</sub>, of
a densely grafted polymer brush of chain length <i>N</i> and grafting density Ď swollen in vapor agrees quantitatively
with the scaling reported by Kuhl et al. for densely grafted brushes
swollen in liquid. Deep in the brush, next to the substrate, the shape
of the segment concentration profile is the same whether the brush
is swollen by liquid or by vapor. Differences in the segment concentration
profile are manifested primarily in the swollen brush interface with
the surrounding fluid. The interface of the polymer brush swollen
in vapor is much more abrupt than that of the same brush swollen in
liquid. This has implications for the compressibility of the swollen
brush surface and for fluctuations at that surface
Loading and Distribution of a Model Small Molecule Drug in Poly(<i>N</i>âisopropylacrylamide) Brushes: a Neutron Reflectometry and AFM Study
The
structure of a hydrated polyÂ(<i>N</i>-isopropylacrylamide)
brush loaded with 5 vol % Isoniazid is studied as a function of temperature
using neutron reflectometry (NR) and atomic force microscopy (AFM).
NR measurements show that Isoniazid increases the thickness of the
brush before, during and after
the polymer collapse, and it is retained inside the brush at all measured
temperatures. The Isoniazid concentration in the expanded brush is
âź14% higher than in the bulk solution, and the concentration
nearly doubles in the collapsed polymer, suggesting stronger binding
between Isoniazid and the polymer compared to water, even at temperatures
below the lower critical solution temperature (LCST) where the polymer
is hydrophilic. Typically, additives that bind strongly to the polymer
backbone and increase the hydrophilicity of the polymer will delay
the onset of the LCST, which is suggested by AFM and NR measurements.
The extent of small-molecule loading and distribution throughout a
thermo-responsive polymer brush, such as pNIPAAm, will have important
consequences for applications such as drug delivery and gating
Structure of [C<sub>4</sub>mpyr][NTf<sub>2</sub>] Room-Temperature Ionic Liquid at Charged Gold Interfaces
The structure of 1-butyl-1-methylpyrrolidinium bisÂ(trifluoromethylsulfonyl)Âimide
([C<sub>4</sub>mpyr]Â[NTf<sub>2</sub>]) room-temperature ionic liquid
at an electrified gold interface was studied using neutron reflectometry,
cyclic voltammetry, and differential capacitance measurements. Subtle
differences were observed between the reflectivity data collected
on a gold electrode at three different applied potentials. Detailed
analysis of the fitted reflectivity data reveals an excess of [C<sub>4</sub>mpyr]<sup>+</sup> at the interface, with the amount decreasing
at increasingly positive potentials. A cation rich interface was found
even at a positively charged electrode, which indicates a nonelectrostatic
(specific) adsorption of [C<sub>4</sub>mpyr]<sup>+</sup> onto the
gold electrode
Structure of [C<sub>4</sub>mpyr][NTf<sub>2</sub>] Room-Temperature Ionic Liquid at Charged Gold Interfaces
The structure of 1-butyl-1-methylpyrrolidinium bisÂ(trifluoromethylsulfonyl)Âimide
([C<sub>4</sub>mpyr]Â[NTf<sub>2</sub>]) room-temperature ionic liquid
at an electrified gold interface was studied using neutron reflectometry,
cyclic voltammetry, and differential capacitance measurements. Subtle
differences were observed between the reflectivity data collected
on a gold electrode at three different applied potentials. Detailed
analysis of the fitted reflectivity data reveals an excess of [C<sub>4</sub>mpyr]<sup>+</sup> at the interface, with the amount decreasing
at increasingly positive potentials. A cation rich interface was found
even at a positively charged electrode, which indicates a nonelectrostatic
(specific) adsorption of [C<sub>4</sub>mpyr]<sup>+</sup> onto the
gold electrode
Structure of [C<sub>4</sub>mpyr][NTf<sub>2</sub>] Room-Temperature Ionic Liquid at Charged Gold Interfaces
The structure of 1-butyl-1-methylpyrrolidinium bisÂ(trifluoromethylsulfonyl)Âimide
([C<sub>4</sub>mpyr]Â[NTf<sub>2</sub>]) room-temperature ionic liquid
at an electrified gold interface was studied using neutron reflectometry,
cyclic voltammetry, and differential capacitance measurements. Subtle
differences were observed between the reflectivity data collected
on a gold electrode at three different applied potentials. Detailed
analysis of the fitted reflectivity data reveals an excess of [C<sub>4</sub>mpyr]<sup>+</sup> at the interface, with the amount decreasing
at increasingly positive potentials. A cation rich interface was found
even at a positively charged electrode, which indicates a nonelectrostatic
(specific) adsorption of [C<sub>4</sub>mpyr]<sup>+</sup> onto the
gold electrode
Structure of [C<sub>4</sub>mpyr][NTf<sub>2</sub>] Room-Temperature Ionic Liquid at Charged Gold Interfaces
The structure of 1-butyl-1-methylpyrrolidinium bisÂ(trifluoromethylsulfonyl)Âimide
([C<sub>4</sub>mpyr]Â[NTf<sub>2</sub>]) room-temperature ionic liquid
at an electrified gold interface was studied using neutron reflectometry,
cyclic voltammetry, and differential capacitance measurements. Subtle
differences were observed between the reflectivity data collected
on a gold electrode at three different applied potentials. Detailed
analysis of the fitted reflectivity data reveals an excess of [C<sub>4</sub>mpyr]<sup>+</sup> at the interface, with the amount decreasing
at increasingly positive potentials. A cation rich interface was found
even at a positively charged electrode, which indicates a nonelectrostatic
(specific) adsorption of [C<sub>4</sub>mpyr]<sup>+</sup> onto the
gold electrode
Water Is a Poor Solvent for Densely Grafted Poly(ethylene oxide) Chains: A Conclusion Drawn from a Self-Consistent Field Theory-Based Analysis of Neutron Reflectivity and Surface PressureâArea Isotherm Data
By use of a combined experimental and theoretical approach,
a model
polyÂ(ethylene oxide) (PEO) brush system, prepared by spreading a polyÂ(ethylene
oxide)âpolyÂ(<i>n</i>-butyl acrylate) (PEOâPnBA)
amphiphilic diblock copolymer onto an airâwater interface,
was investigated. The polymer segment density profiles of the PEO
brush in the direction normal to the airâwater interface under
various grafting density conditions were determined by using the neutron
reflectivity (NR) measurement technique. To achieve a theoretically
sound analysis of the reflectivity data, we used a data analysis method
that utilizes the self-consistent field (SCF) theoretical modeling
as a tool for predicting expected reflectivity results for comparison
with the experimental data. Using this data analysis technique, we
discovered that the effective FloryâHuggins interaction parameter
of the PEO brush chains is significantly greater than that corresponding
to the θ condition in FloryâHuggins solutions (i.e.,
Ď<sub>PEOâwater</sub>(brush chains)/Ď<sub>PEOâwater</sub>(θ condition) â 1.2), suggesting that contrary to what
is more commonly observed for PEO in normal situations (Ď<sub>PEOâwater</sub>(free chains)/Ď<sub>PEOâwater</sub>(θ condition) â 0.92), the PEO chains are actually not
âhydrophilicâ when they exist as polymer brush chains,
because of the many body interactions that are forced to be effective
in the brush situation. This result is further supported by the fact
that the surface pressures of the PEO brush calculated on the basis
of the measured Ď<sub>PEOâwater</sub> value are in close
agreement with the experimental surface pressureâarea isotherm
data. The SCF theoretical analysis of the surface pressure behavior
of the PEO brush also suggests that even though the grafted PEO chains
experience a poor solvent environment, the PEO brush layer exhibits
positive surface pressures, because the hydrophobicity of the PEO
brush chains (which favors compression) is insufficient to overcome
the opposing effect of the chain conformational entropy (which resists
compression)