15 research outputs found
Release Behavior of Polymeric Vesicles in Solution Controlled by External Electrostatic Field
We
found that the polymeric vesicles from the self-assembly of
amphiphilic block copolymer polystyrene-<i>block</i>-polyÂ(acrylic
acid) (PS<sub>144</sub>-<i>b</i>-PAA<sub>22</sub>) in the
dioxane/water mixture can be deformed, broken and finally divided
into smaller ones via the external electrostatic field. The higher
the electrostatic field intensity, the smaller the vesicles. More
importantly, this fission phenomenon induced by electrostatic field
can be used to control the release behavior of the vesicles. Our experimental
results show that the Nile Red (NR) molecules encapsulated inside
the cavity of vesicles can be accurately released by controlling the
electrostatic field intensity and the release time. These findings
not only enrich the knowledge for the external field induced transformation
of polymer structures, but also provide a new and highly convenient
approach for the controllable release of polymersomes in solution
Design of Electrical Conductive Composites: Tuning the Morphology to Improve the Electrical Properties of Graphene Filled Immiscible Polymer Blends
Polystyrene (PS) and polyÂ(methyl methacrylate) (PMMA)
blends filled
with octadecylamine-functionalized graphene (GE-ODA) have been fabricated
to obtain conductive composites with a lower electrical percolation
threshold according to the concept of double percolation. The dependence
of the electrical properties of the composites on the morphology is
examined by changing the proportion of PS and PMMA. Our results reveal
that the electrical conductivity of the composites can be optimal
when PS and PMMA phases form a cocontinuous structure and GE-ODA nanosheets
are selectively located and percolated in the PS phase. For the PS/PMMA
blend (50w/50w), the composites exhibit an extremely low electrical
percolation threshold (0.5 wt %) because of the formation of a perfect
double percolated structure. Moreover, the rheological properties
of the composites are also measured to gain a fundamental understanding
of the relationship between microstructure and electrical properties
Self-Assembly of AB Diblock Copolymer Confined in a Soft Nano-Droplet: A Combination Study by Monte Carlo Simulation and Experiment
The
self-assembly of AB-type diblock copolymers confined in a three-dimensional
(3D) soft nanodroplet is investigated by the combination of Monte
Carlo simulation and experiment. The influences of two critical factors,
i.e., confinement degree of the imposed confinement space and the
interfacial interaction between each individual block and boundary
interface, on the 3D soft confined self-assembly are examined systematically.
The simulation results reveal that block copolymer chains become more
and more folded as the confinement degree (it can be monitored by
the ratio of <i>D</i>/<i>L</i>, where <i>L</i> is the length of polymer chain and <i>D</i> is
the reduced diameter of the final polymeric particle) is enhanced,
causing a series of morphological transitions. Based on the simulation
prediction, we perform the corresponding experiments by the 3D confined
self-assembly of both symmetric and asymmetric block copolymers within
the emulsion droplets. The experimental results well reproduce the
confinement degree induced morphological transitions predicted by
the simulations, such as the transition from segmented pupa-like particle
to hamburger particle and the transition from raspberry-like particle
to triangle-like particle, and then to hamburger particle. The current
study implies that self-assembled nanostructures under 3D soft confinement
can be simply controlled by tuning the confinement degree and interfacial
property, i.e., the ratio of <i>D</i>/<i>L</i> and the interfacial interaction between each individual block and
boundary interface
Controllable Cooperative Self-Assembly of PS‑<i>b</i>‑PAA/PS‑<i>b</i>‑P4VP Mixture by Tuning the Intercorona Interaction
The cooperative self-assembly of
amphiphilic polystyrene-<i>block</i>-polyÂ(acrylic acid)
(PS<sub>144</sub>-<i>b</i>-PAA<sub>22</sub>) and polystyrene-<i>block</i>-polyÂ(4-vinylpyridine)
(PS<sub>144</sub>-<i>b</i>-P4VP<sub>33</sub>) diblock copolymers
in DMF/H<sub>2</sub>O mixtures has been investigated. Both copolymers
self-assemble into small spherical micelles (SSMs) if used individually.
However, the equimolar mixture of these two copolymers cooperatively
self-assembles into vesicles. It is found that the formation of vesicles
is attributed to the complex interactions between PAA and P4VP chains,
including the hydrogen bonds between un-ionized acrylic acid units
and pyridine units as well as the electronic attractions between ionized
acrylic acid units and protonated pyridine units. Since these interactions
between PAA and P4VP chains depend on pH value, the cooperatively
self-assembled morphology can be easily tuned by the addition of HCl
or NaOH. At high addition of H<sup>+</sup> or OH<sup>–</sup>, the intercorona interaction is repulsive and the copolymer mixture
tends to form SSMs (basic condition) or cylindrical micelles (acidic
condition), whereas it prefers to aggregate into vesicles at low addition
of H<sup>+</sup> or OH<sup>–</sup> because the intercorona
interaction is attractive. Interestingly, the same morphology of the
self-assembled aggregates can be obtained either at high H<sup>+</sup> addition or at low OH<sup>–</sup> addition, which results
from the nonmonotonic variation of the intercorona interaction along
with the addition of HCl or NaOH. The current study implies that it
is the intercorona interaction rather than the chemical condition
that dominates the cooperatively self-assembled morphology
Online Rheological Investigation on Ion-Induced Micelle Transition for Amphiphilic Polystyrene-<i>block</i>-Poly(acrylic acid) Diblock Copolymer in Dilute Solution
The ion-induced micellar transition
is online-investigated by the
time dependence of the viscosity of the solution under shear flow
for the first time. During the morphological transition, the change
in the micellar structure can be tracked by the change in viscosity.
Adding HCl or CaCl<sub>2</sub> into pre-prepared spherical micelle
solution from the self-assembly of polystyrene-<i>block</i>-polyÂ(acrylic acid) (PS<sub>144</sub>-<i>b</i>-PAA<sub>22</sub>) in the <i>N</i>,<i>N</i>-dimethylformamide
(DMF)/water mixture, the micellar structures change into short cylinders,
long, entangled cylinders, and then lamellae or vesicles, corresponding
to the viscosity increasing first and then declining. When HCl or
CaCl<sub>2</sub> is added to the pre-prepared spherical micelle solution
formed by PS<sub>144</sub>-<i>b</i>-PAA<sub>50</sub> in
the dioxane/water mixture, the micellar structures are quickly transformed
into cylinders or lamellae before carrying out the rheological measurement
and then are turned to vesicles or spheres under the shearing, corresponding
to a gradual decline in viscosity. This study shows that the rheology
can be a very simple and effective online method on the investigation
of the micellization, which plays an important role in understanding
the micellization mechanism and micellar transition pathway of block
copolymers in dilute solution
Shear Flow Controlled Morphological Polydispersity of Amphiphilic ABA Triblock Copolymer Vesicles
Self-assembled
polymeric aggregates are generally polydisperse in morphology due
to the existence of many metastable states in the system. This shortcoming
becomes a bottleneck for preparing high quality self-assembled polymeric
materials. An important concern is the possibility of controlling
morphological polydispersity through the modulation of the metastable
states. In this study, both simulative and experimental results show
that the metastable states can be modulated. As a typical example,
the morphological polydispersity of amphiphilic ABA triblock copolymer
vesicles have been successfully controlled by shear flow. A higher
shear rate results in more uniform and smaller vesicles. However,
if the shear rate is extremely high, small spheres and short rods
can be observed. These findings not only give a deeper insight into
the metastable behavior of self-assembled polymeric aggregates but
also provide a new strategy for improving the uniformity of vesicles
Entropy-Driven Hierarchical Nanostructures from Cooperative Self-Assembly of Gold Nanoparticles/Block Copolymers under Three-Dimensional Confinement
The
cooperative self-assembly of polystyrene-<i>b</i>-polyÂ(4-vinylpyridine)
block copolymers (BCPs) and gold nanoparticles
(AuNPs) confined within the emulsion droplets is studied by combining
both the experiments and Monte Carlo simulations. The results indicate
that the entropic interaction between the AuNPs and BCP domain is
a critical parameter to dominate the spatial arrangement of AuNPs
and the nanostructure of the hybrid nanoparticles, which can be utilized
to design novel hierarchical hybrid nanoparticles. Based on this theoretical
observation, a large number of unique Janus hybrid nanoparticles,
including pupa-like nanoparticles with AuNPs concentrated at one pole
of the particles, spherical nanoparticles with AuNPs enriched in a
bulge on the sphere surface, and the gourd-like, clover-like, and
four-leaf-clover-like nanoparticles from the further hierarchical
assembly of small hybrid Janus nanoparticles, are fabricated via three-dimensional
(3D) confined self-assembly
Inorganic Nanoparticle Induced Morphological Transition for Confined Self-Assembly of Block Copolymers within Emulsion Droplets
Recently,
it has been reported that the incorporation of functional
inorganic nanoparticles (NPs) into the three-dimensional (3D) confined
self-assembly of block copolymers (BCPs) creates the unique nanostructured
hybrid composites, which can not only introduce new functions to BCPs
but also induce some interesting morphological transitions of BCPs.
In the current study, we systematically investigate the cooperative
self-assembly of a series of size-controlled and surface chemistry-tunable
gold nanoparticles (AuNPs) and polystyrene-<i>b</i>-polyÂ(2-vinylpyridine)
(PS-<i>b</i>-P2VP) diblock copolymer within the emulsion
droplets. The influences of the size, content, and surface chemistry
of the AuNPs on the coassembled nanostructures as well as the spatial
distribution of AuNPs in the hybrid particles are examined. It is
found that the size and content of the AuNPs are related to the entropic
interaction, while the surface chemistry of AuNPs is related to the
enthalpic interaction, which can be utilized to tailor the self-assembled
morphologies of block copolymer confined in the emulsion droplets.
As the content of PS-coated AuNPs increases, the morphology of the
resulting AuNPs/PS-<i>b</i>-P2VP hybrid particles changes
from the pupa-like particles to the bud-like particles and then to
the onion-like particles. However, a unique morphological transition
from the pupa-like particles to the mushroom-like particles is observed
as the content of P4VP-coated AuNPs increases. More interestingly,
it is observed that the large AuNPs are expelled to the surface of
the BCP particles to reduce the loss in the conformational entropy
of the block segment, which can arrange into the strings of necklaces
on the surfaces of the hybrid particles
Controllable Location of Inorganic Nanoparticles on Block Copolymer Self-Assembled Scaffolds by Tailoring the Entropy and Enthalpy Contributions
Precisely
controlling the spatial location and alignment of functional
nanoparticles (NPs) on polymeric scaffolds is of great importance
to not only create novel nanostructures but also enhance the properties
of the hybrid nanomaterials. Herein, we demonstrate a strategy of
tailoring the entropic and enthalpic contributions to precisely position
gold nanoparticles (AuNPs) on block copolymer (BCP) scaffolds through
the confined coassembly of BCPs and AuNPs within the emulsion droplet.
According to this strategy, entropic effect arisen by the loss in
conformational entropy and the enthalpic attraction between ligands
on AuNPs and surfactants at the oil/water interface induce the solid
AuNPs to move to the BCP surface, while the enthalpic interaction
between the ligands on AuNPs and the corresponding polymer chains
guides the AuNPs to position at the appropriate place. By this strategy,
both the location and alignment of AuNPs on BCP scaffolds can be controlled
at will, such as at the two terminals or along the lamellar boundary
of the pupa-like scaffolds, or at the bases of pinecone-like or bud-like
scaffolds, or at the head of one hemisphere, the entire hemisphere,
or along the boundary between the two distinct hemispheres of the
Janus-like scaffolds. We believe that this methodology can offer a
universal route to achieve the precise positioning of functional NPs
on the BCP scaffolds
Parallel Carbon Nanotube Stripes in Polymer Thin Film with Remarkable Conductive Anisotropy
In
our previous study (Mao et al. J. Phys. Chem. Lett. 2013, 4, 43−47), we proposed
a novel method, that is, the shear-flow-induced hierarchical self-assembly
of two-dimensional fillers (octadecylamine-functionalized graphene)
into the well-ordered parallel stripes in a polymer matrix, to fabricate
the anisotropic conductive materials. In this study, we extend this
method to one-dimensional multiwalled carbon nanotubes (MWCNTs). Under
the induction of shear flow, the dispersed polyÂ(styrene ethylene/butadiene-styrene)
(SEBS) phase and MWCNTs can spontaneously assemble into well-ordered
parallel stripes in the polypropylene (PP) thin film. The electrical
measurements indicate that the electrical resistivity in the direction
parallel to the stripes is almost 6 orders of magnitude lower than
that in the perpendicular direction, which is by far the most striking
conductive anisotropy for the plastic anisotropic conductive materials.
In addition, it is found that the size of the MWCNT stripe as well
as the electrical property of the resulting anisotropic conductive
thin film can be well-controlled by the gap of the shear cell