12 research outputs found
Observation of Water-Stimulated Supercontraction of Uniaxially Oriented Poly(vinyl alcohol) and the Related Hierarchical Structure Change Revealed by the Time-Resolved WAXD/SAXS Measurements
A uniaxially oriented polyÂ(vinyl
alcohol) (PVA) film was found
for the first time to respond to the humidity change in the two different
modes under the restrained condition, which are essentially the same
as the modes of the supercontraction and cyclic contraction observed
in spider dragline silk. Once the atmospheric humidity started to
increase, the PVA film showed at first the irreversible stress generation
(supercontraction stress), followed by the reversible stress generation
synchronizing with the cyclic change of humidity. These irreversible
and reversible stress changes have been connected to the changes of
higher-order structure caused by the cyclic change of wet/dry atmosphere
as revealed by the detailed <i>in situ</i> measurements
of the 2-dimensional wide-angle and small-angle X-ray scatterings
during these processes. On the basis of a simple mechanical model
and the thus-collected information on the higher-order structural
change, it was concluded that the irreversible and reversible stress
generations are governed mainly by the irreversible hydration-induced
stress relaxation in the highly tensioned amorphous region and the
reversible swelling in the normal amorphous region, respectively
Fully Liquid-Crystalline ABA Triblock Copolymer of Fluorinated Side-Chain Liquid-Crystalline A Block and Main-Chain Liquid-Crystalline B Block: Higher Order Structure in Bulk and Thin Film States
Fully liquid-crystalline (LC) ABA-type
triblock copolymers were synthesized by atom transfer radical polymerization;
the A block was a fluorinated side-chain LC polymer, PFA-C<sub>8</sub>, and the B block was a main-chain LC polyester, BB-5Â(3-Me). The
volume fraction of the A block (φ<sub>A</sub>) was 0.11–0.70,
and the B block had a constant molecular weight. Nanometer-scale segregated
structures in the bulk and thin film states were investigated by synchrotron
X-ray diffraction (XRD) in transmission and grazing-incidence (GI)
geometries to examine the effect of competition between the LC orientation
and polymer chain dimensions on the morphology. When φ<sub>A</sub> is 0.11, matching of the mesogen orientation in the A and B blocks
dominates the main-chain orientation, whereas when φ<sub>A</sub> exceeds 0.28, matching of the lateral dimensions of the A and B
blocks dominates the mesogen orientation, although all the polymers
showed lamellar structure before isotropization of BB-5Â(3-Me). GI-XRD
revealed that the lamellar structure in the thin film with φ<sub>A</sub> = 0.70 was completely perpendicular to the Si substrate without
surface modification or solvent annealing
Transformation of Coiled α‑Helices into <i>Cross</i>-β-Sheets Superstructure
The
fibrous silk produced by bees, wasps, ants, or hornets is known
to form a four-strand α-helical coiled coil superstructure.
We have succeeded in showing the formation of this coiled coil structure
not only in natural fibers, but also in artificial films made of regenerated
silk of the hornet <i>Vespa simillima xanthoptera</i> using
wide- and small-angle X-ray scatterings and polarized Fourier transform
infrared spectroscopy. On the basis of time-resolved simultaneous
synchrotron X-ray scattering observations for in situ monitoring of
the structural changes in regenerated silk material during tensile
deformation, we have shown that the application of tensile force under
appropriate conditions induces a transition from the coiled α-helices
to a <i>cross</i>-β-sheet superstructure. The four-stranded
tertiary superstructure remains unchanged during this process. It
has also been shown that the amorphous protein chains in the regenerated
silk material are transformed into conventional β-sheet arrangements
with varying orientation
Design of High-Density Helical Polymer Brush on Silica Nanoparticles for the Size Recognition of Fullerene Molecules
High-density
syndiotactic polyÂ(methyl methacrylate) (<i>st-</i>PMMA)
brushes form a helical structure and encapsulate fullerene
molecules in their helical cavities, leading to a PMMA brush/fullerene
inclusion complex. The brushes recognize the size of guest molecules
and spontaneously adapt their helical diameter to the guest molecules.
Both polymer brush/C<sub>60</sub> and polymer brush/C<sub>70</sub> inclusion complex on the flat substrate were characterized on the
basis of grazing incidence wide-angle X-ray diffraction (GIWAXD) measurements,
and it is revealed that the main chains oriented perpendicular to
the substrate. Moreover, high-density <i>st</i>-PMMA brushes
grafted onto nanoparticles efficiently separate C<sub>70</sub> molecules
from the mixture of C<sub>60</sub> and C<sub>70</sub> solution. Even
after 5× repeating process, the selectivity for C<sub>70</sub> molecules remains at 99%
Confinement-Induced Crystal Growth in One-Dimensional Isotactic Polystyrene Nanorod Arrays
This work demonstrates the anomalous
crystal growth of isotactic
polystyrene (iPS) in nanorod arrays with different rod sizes. At the
bottom of the nanorods, the crystals in bulk film grow into nanorods
along either the [110] or [100] direction parallel to the rod axis.
On the top side of the nanorods, the polymer exhibits different orientations
corresponding to weak or strong confinement. In the weaker confinement
(bigger nanorods of 300 nm diameter), the crystals grow with the [100]
direction along the nanorod, which is similar to the crystals developed
in the radial of spherulite. In the stronger confinement (smaller
nanorods of 65 nm diameter), the splaying of crystals in the rod is
significantly suppressed, and the preferred growth direction of iPS
crystals is kept in either the [110] or [100] direction. The precise
control of polymer crystal orientation and crystallinity at a local
scale opens important perspectives for the design of one-dimensional
nanomaterials whose performance depends on the anisotropic crystal
properties
Salt Dependence of the Chain Stiffness and Excluded-Volume Strength for the Polymethacrylate-Type Sulfopropylbetaine in Aqueous NaCl Solutions
A series of zwitterionic polyelectrolytes
polyÂ[3-(<i>N</i>-2-methacrylÂoyloxyÂethyl-<i>N</i>,<i>N</i>-dimethyl)ÂammonatoÂpropaneÂsulfonate]
(PMAPS) with
a wide range of weight-average molecular weight (<i>M</i><sub>w</sub>) between 5.5 × 10<sup>3</sup> and 1.6 × 10<sup>6</sup> g mol<sup>–1</sup> with narrow molecular weight distribution
(<i>M</i><sub>w</sub>/<i>M</i><sub>n</sub> = 1.07–1.19)
were thoroughly characterized in aqueous NaCl solutions for salt concentration
(<i>C</i><sub>s</sub>) over a range from theta <i>C</i><sub>s</sub> (0.074 M) to 1.0 M by synchrotron radiation small-angle
X-ray scattering (SAXS), light scattering, and viscometry at 25 °C.
To determine the chain stiffness parameter (λ<sup>–1</sup>) and the excluded-volume strength (<i>B</i>) of PMAPS
in an aqueous NaCl solution, SAXS profiles and the <i>M</i><sub>w</sub> dependences of the radius of gyration, the second virial
coefficient, the interpenetration function, the hydrodynamic radius,
and the intrinsic viscosity for PMAPS were analyzed on the basis of
the (un)Âperturbed cylindrical wormlike chain model. The experimental
λ<sup>–1</sup> value for PMAPS chains in aqueous NaCl
solutions barely decreased but was almost constant with the increasing <i>C</i><sub>s</sub>, whereas the value of <i>B</i> was
increased gradually with the increasing <i>C</i><sub>s</sub>. Thus, the dominant factor for the chain dimension of PMAPS in aqueous
NaCl solutions was the long-range interaction (i.e., <i>B</i>) than the short-range interaction (i.e., λ<sup>–1</sup>). The observed <i>C</i><sub>s</sub> dependences of λ<sup>–1</sup> and <i>B</i> for PMAPS chains in aqueous
NaCl solutions were fairly described by the theories of the polyampholyte
with the nonrepulsive, the repulsive, and the attractive electrostatic
interactions
Molecular Aggregation States and Physical Properties of Syndiotactic Polystyrene/Hydrogenated Polyisoprene Multiblock Copolymers with Crystalline Hard Domain
Molecular
aggregation structure and mechanical as well as thermal
properties of novel well-defined multiblock copolymers consisting
of crystalline syndiotactic polystyrene (sPS) and rubbery hydrogenated
polyisoprene (hPIp) were investigated. The morphology and crystalline
ordered structure of the multiblock copolymer films prepared by solvent
casting from 1,2-dichlorobenzene solution depended on the volume fraction
of sPS (VF<sub>sPS</sub>) and number of blocks. The multiblock copolymer
films exhibited ordered morphology with low crystallinity. The crystallinity
of the sPS reduced with decreasing the VF<sub>sPS</sub>. The pentablock
copolymer produced more ordered morphology and less crystallinity
than the triblock copolymers. The anisotropic orientation and mechanical
stability of the δ form sPS crystals in the spherical sPS domains
during uniaxial stretching were demonstrated. Tensile testing and
dynamic mechanical analysis indicated that these multiblock copolymer
films with appropriate sPS fraction are strong, tough, and elastic
and thus could be potential candidates for a new type of thermoplastic
elastomer with discrete crystalline hard domains
Hierarchical Structural Change in the Stress-Induced Phase Transition of Poly(tetramethylene terephthalate) As Studied by the Simultaneous Measurement of FTIR Spectra and 2D Synchrotron Undulator WAXD/SAXS Data
The simultaneous measurement of Fourier
transform infrared (FTIR)
transmission spectra and 2-dimensional wide-angle X-ray diffraction
(WAXD) and small-angle X-ray scattering (SAXS) patterns has been performed
successfully to investigate the hierarchical structure changes occurring
in the stress-induced phase transition phenomenon of uniaxially oriented
polyÂ(tetramethylene terephthalate) film. The molar fraction of the
β-crystal form, evaluated from the IR and WAXD data analyses,
increased steeply in the plateru region of the stress–strain
curve as already known well. The 2D SAXS data have revealed the remarkable
and reversible change in the stacked lamellar structure just after
the α-to-β phase transition was completed, where the tilting
angle of the stacked lamellae measured from the draw axis of the oriented
sample became zero, and the lamellar thickness increased due to the
inclusion of amorphous region located in the boundary part of the
crystalline lamellae. In parallel, the X-ray reflection spots in a
wider diffraction angle region became diffuse in the observed WAXD
pattern of the β form, indicating the packing disorder of the
mechanically stressed chains. In this way, the simultaneous combination
of the 3 different types of equipments has allowed us to deduce the
detailed structural change from the various levels: the stress-induced
α–β transition was found to occur not only with
the remarkable changes in the molecular chain conformation and chain
packing mode in the crystal lattice, but also with the large and reversible
change in the lamellar stacking structure. The stress-induced changes
in lamellar thickness and long period were simulated using a mechanical
model with these hierarchical structure changes taken into account,
giving relatively good reproduction of the observed data
Hydrophobic Molecules Infiltrating into the Poly(ethylene glycol) Domain of the Core/Shell Interface of a Polymeric Micelle: Evidence Obtained with Anomalous Small-Angle X‑ray Scattering
Polymeric micelles have been extensively studied as nanoscale
drug
carriers. Knowing the inner structure of polymeric micelles that encapsulate
hydrophobic drugs is important to design effective carriers. In our
study, the hydrophobic compound tetrabromocathecol (TBC) was chosen
as a drug-equivalent model molecule. The bromine atoms in TBC act
as probes in anomalous small-angle X-ray scattering (ASAXS) allowing
for its localization in the polymeric micelles whose shape and size
were determined by normal small-angle X-ray scattering (SAXS). Light
scattering measurements coupled with field flow fractionation were
also carried out to determine the aggregation number of micelles.
A core–corona spherical model was used to explain the shape
of the micelles, while the distribution of bromine atoms was explained
with a hard-sphere model. Interestingly, the radius of the spherical
region populated with bromine atoms was larger than the one of the
sphere corresponding to the hydrophobic core of the micelle. This
result suggests that the TBC molecules infiltrate the PEG hydrophilic
domain in the vicinity of the core/shell interface. The results of
light scattering and SAXS indicate that the PEG chains at the shell
region are densely packed, and thus the PEG domain close to the interface
has enough hydrophobicity to tolerate the presence of hydrophobic
compounds
Depth-Resolved Characterization of Perylenediimide Side-Chain Polymer Thin Film Structure Using Grazing-Incidence Wide-Angle X‑ray Diffraction with Tender X‑rays
Polymers
with a perylenediimide (PDI) side chain (PAc12PDI) consist
of two kinds of crystalline structures with various types of orientations
in a thin film. Understanding the population of the microcrystalline
structure and its orientation along the thickness is strongly desired.
Grazing-incidence wide-angle X-ray diffraction (GIWAXD) measurements
with hard X-rays, which are generally chosen as λ = 0.1 nm,
are a powerful tool to evaluate the molecular aggregation structure
in thin films. A depth-resolved analysis for the outermost surface
of the polymeric materials using conventional GIWAXD measurements,
however, has limitations on depth resolution because the X-ray penetration
depth dramatically increases above the critical angle. Meanwhile,
tender X-rays (λ = 0.5 nm) have the potential advantage that
the penetration depth gradually increases above the critical angle,
leading to precise characterization for the population of crystallite
distribution along the thickness. The population of the microcrystalline
states in the PAc12PDI thin film was precisely characterized utilizing
GIWAXD measurements using tender X-rays. The outermost surface of
the PAc12PDI thin film is occupied by a monoclinic lattice with <i>a</i> = 2.38 nm, <i>b</i> = 0.74 nm, <i>c</i> = 5.98 nm, and β = 108.13°, while maintaining the <i>c-</i>axis perpendicular to the substrate surface. Additionally,
the presence of solid substrate controls the formation of the crystallite
with unidirectional orientation