25 research outputs found
Speeding of Spherulitic Growth Rate at the Late Stage of Isothermal Crystallization Due to Interfacial Diffusion for Double-Layer Semicrystalline Polymer Films
In
this study a unique phenomenon has been found for isothermal crystallization
of double-layer semicrystalline polymer films. It is surprisingly
found that there exists a speeding of polyÂ(l-lactic acid)
(PLA) spherulitic growth rate for polyÂ(ethylene oxide)/polyÂ(l-lactic acid) (PEO/PLA) double-layer films at the late stage of isothermal
crystallization, which does not exist for PLA/PEO blend films and
neat PLA films. The mutual diffusion between PEO and PLA layers plays
the key factor to bring out the observed speeding of spherulitic growth
rate. This type of study provides an avenue for understanding the
interplay between polymer crystallization and interfacial diffusion
in multilayer polymer films, which is not available when employing
the polymer blend films
Bioinspired Design of Nanostructured Elastomers with Cross-Linked Soft Matrix Grafting on the Oriented Rigid Nanofibers To Mimic Mechanical Properties of Human Skin
Human skin exhibits highly nonlinear elastic properties that are essential to its physiological functions. It is soft at low strain but stiff at high strain, thereby protecting internal organs and tissues from mechanical trauma. However, to date, the development of materials to mimic the unique mechanical properties of human skin is still a great challenge. Here we report a bioinspired design of nanostructured elastomers combining two abundant plant-based biopolymers, stiff cellulose and elastic polyisoprene (natural rubber), to mimic the mechanical properties of human skin. The nanostructured elastomers show highly nonlinear mechanical properties closely mimicking that of human skin. Importantly, the mechanical properties of these nanostructured elastomers can be tuned by adjusting cellulose content, providing the opportunity to synthesize materials that mimic the mechanical properties of different types of skins. Given the simplicity, efficiency, and tunability, this design may provide a promising strategy for creating artificial skin for both general mechanical and biomedical applications
Bioinspired High Resilient Elastomers to Mimic Resilin
Natural resilin possesses outstanding
mechanical properties, such
as high strain, low stiffness, and high resilience, which are difficult
to be reproduced in synthetic materials. We designed high resilient
elastomers (HREs) with a network structure to mimic natural resilin
on the basis of two natural abundant polymers, stiff cellulose and
flexible polyisoprene. With plasticization via mineral oil and mechanical
cyclic tensile deformation processing, HREs show ultrahigh resilience,
high strain, and reasonable tensile strength that closely mimic natural
resilin. Moreover, the mechanical properties of HREs can be finely
tuned by adjusting the cellulose content, providing the opportunity
to synthesize high resilient elastomers that mimic different elastic
proteins, such as elastin
Preparation of Novel Cross-Linked and Octylated Caseinates Using a Biphasic Enzymatic Procedure and Their Functional Properties
A novel
microbial transglutaminase-catalyzed aqueous–organic
biphasic reaction system was successfully developed to prepare caseinate
derivatives by cross-linking and incorporating nonpolar octyl tails
for the first time. SDS-PAGE and <sup>1</sup>H NMR analysis confirmed
that cross-linking and octyl conjugation occurred simultaneously.
The octyl substitution degree (SD) was measured by <sup>1</sup>H NMR
and used as an index to determine a suitable reaction condition. It
was found that at the condition of 0.125% (w/v) protein concentration
and 6 h of reaction time, the modified caseinate had the highest SD
of 28.96%. The modified caseinate also had an increased surface hydrophobicity,
better emulsifying activity, and improved thermal and salt stabilities.
However, its emulsion stability or in vitro enzymatic digestibility
was slightly lower than that of the native caseinate
Critical Content of Ultrahigh-Molecular-Weight Polyethylene To Induce the Highest Nucleation Rate for Isotactic Polypropylene in Blends
The influence of the addition of low amounts of ultrahigh-molecular-weight
polyethylene (UHMWPE) on the crystallization kinetics of isotactic
polypropylene (iPP) in iPP/UHMWPE blends has been investigated by
means of differential scanning calorimetry (DSC) and polarized optical
microscopy. During the nonisothermal crystallization process, the
primarily formed UHMWPE crystals serve as heterogeneous nucleating
agents for iPP nucleation, whereas during the isothermal crystallization
process, UHMWPE is in the molten state, iPP nucleation preferentially
occurs at the UHMWPE and iPP phase interfaces, and the spherulitic
growth rates are not obviously affected. It is particularly interesting
to find a critical UHMWPE content (2.5 wt %) in the blends to induce
the highest iPP nucleation rate; however, above the critical UHMWPE
content, the iPP nucleation rate slows because of aggregation of the
UHMWPE component. A delicately designed DSC measurement provides insight
into the nucleation mechanism of iPP at the interfaces between the
UHMWPE and iPP phase domains. It is proposed that the concentration
fluctuations generated from the unstable inhomogeneous phase interfaces
in the iPP/UHMWPE blends promote the formation of nuclei, which eventually
enhances the nucleation and overall crystallization rates of the iPP
component
Structural, Thermal, and Anti-inflammatory Properties of a Novel Pectic Polysaccharide from Alfalfa (Medicago sativa L.) Stem
A pectic polysaccharide (APPS) was
purified from the cold alkali
extract of alfalfa stem and characterized to be a rhamnogalacturonan
I (RG-I) type pectin with the molecular weight of 2.38 × 10<sup>3</sup> kDa and a radius of 123 nm. The primary structural analysis
indicated that APPS composed of a →2)-α-l-Rha<i>p</i>-(1→4)-α-d-Gal<i>p</i>A-(1→
backbone with 12% branching point at C-4 of Rha<i>p</i> forming
side chains by l-arabinosyl and d-galactosyl oligosaccharide
units. Transmission electron microscopy (TEM) analysis revealed a
primary linear-shaped structure with a few branches in its assembly
microstructures. The thermal decomposition evaluation revealed the
stability of APPS with an apparent activation energy (<i>E</i><sub>a</sub>) of 226.5 kJ/mol and a pre-exponential factor (<i>A</i>) of 2.10 × 10<sup>25</sup>/s, whereas its primary
degradation occurred in the temperature range from 215.6 to 328.0
°C. In addition, APPS showed significant anti-inflammatory effect
against mRNA expressions of the pro-inflammatory cytokine genes, especially
for IL-1β, suggesting its potential utilization in functional
foods and dietary supplement products
Significantly Accelerated Spherulitic Growth Rates for Semicrystalline Polymers through the Layer-by-Layer Film Method
The
influence of a molten liquid polymer layer on the crystallization
of the beneath semicrystalline polymer has been seldom considered.
In the study, the nucleation and growth of spherulites for the beneath
polylactide (PLA) layer in polyÂ(ethylene oxide)/polylactide (PEO/PLA)
double-layer films during isothermal crystallization at various temperatures
above the melting point of PEO have been investigated by using polarized
optical microscopy, with the particular results compared with that
for neat PLA and PLA/PEO blend films. It is interesting to find that
the top covering molten PEO layer can greatly accelerate the spherulitic
growth rate (<i>G</i>) of the beneath PLA layer. Another
significant result is that the temperature for the measurable nucleation
and spherulitic growth of PLA in the double-layer films can be eventually
pushed down close to the glass transition temperature of neat PLA.
The changes of glass transition temperature, <i>T</i><sub>g</sub>, for PEO/PLA multilayer films have been measured by using
modulated differential scanning calorimetry and dynamic mechanical
analysis, which reveal slight decreases of <i>T</i><sub>g</sub> for PLA layer due to the influence of PEO layer. The layer
structures of fractured surface of the double-layer films are analyzed
on the basis of the observation from scanning electron microscopy,
and the existence of interdiffusion areas with irregular boundary
between PEO and PLA layers is the key clue to understanding the significant
acceleration of <i>G</i> for PLA. The layer-by-layer film
method infers promising applications, which might be considered to
well replace the blending method
Fabrication of Copolymer-Grafted Multiwalled Carbon Nanotube Composite Thermoplastic Elastomers Filled with Unmodified MWCNTs as Additional Nanofillers To Significantly Improve Both Electrical Conductivity and Mechanical Properties
Nanostructured materials have attracted
tremendous attention in
past decades owning to their wide range of potential applications
in many areas. In this study, novel conductive composite thermoplastic
elastomers (CTPEs) were fabricated by using a copolymer-grafted multiwalled
carbon nanotube (MWCNT) composite thermoplastic elastomer filled with
varied amounts of unmodified MWCNTs as additional nanofillers. Rheological
measurements and electrical conductivity tests were performed to investigate
the viscoelasticity and electrical percolation behavior of these CTPEs,
respectively. The incorporation of unmodified MWCNTs can significantly
increase the electrical conductivity of these CTPEs, and the electrical
conductivity percolation threshold was determined to be 0.34 wt %.
The macroscopic mechanical properties of these CTPEs can be conveniently
adjusted by the content of unmodified MWCNTs; for example, the strain-hardening
behavior can be significantly enhanced with the incorporation of unmodified
MWCNTs. This design concept can be generalized to other conductive
composite elastomeric systems
A Novel Alkaline Hemicellulosic Heteroxylan Isolated from Alfalfa (Medicago sativa L.) Stem and Its Thermal and Anti-inflammatory Properties
A novel hemicellulosic polysaccharide
(ACAP) was purified from
the cold alkali extraction of alfalfa stems and characterized as a
heteroxylan with a weight-average molecular weight of 7.94 ×
10<sup>3</sup> kDa and a radius of 58 nm. Structural analysis indicated
that ACAP consisted of a 1,4-linked β-d-Xyl<i>p</i> backbone with 4-<i>O</i>-MeGlc<i>p</i>A and T-l-Ara<i>f</i> substitutions at <i>O</i>-2 and <i>O</i>-3 positions, respectively. Transmission
electron microscopy (TEM) examination revealed the entangled chain
morphology of ACAP molecules. The evaluation of thermal degradation
property revealed a primary decomposition temperature range of 238.8–314.0
°C with an apparent activation energy (<i>E</i><sub>a</sub>) and a pre-exponential factor (<i>A</i>) of 220.0
kJ/mol and 2.81 × 10<sup>24</sup>/s, respectively. ACAP also
showed significant inhibitory activities on IL-1β, IL-6, and
COX-2 gene expressions in cultured RAW 264.7 mouse macrophage cells.
These results suggested the potential utilization of ACAP in functional
foods and dietary supplement products
Thermoactivated Electrical Conductivity in Perylene Diimide Nanofiber Materials
Thermoactivated
electrical conductivity has been studied on nanofibers
fabricated from the derivatives of perylene tetracarboxylic diimide
(PTCDI) both in the dark and under visible light illumination. The
activation energy obtained for the nanofibers fabricated from donor–acceptor
(D–A) PTCDIs are higher than that for symmetric <i>n</i>-dodecyl substituted PTCDI. Such difference originates from the strong
dependence of thermoactivated charge hopping on material disorder,
which herein is dominated by the D–A charge-transfer and dipole–dipole
interactions between stacked molecules. When the nanofibers were heated
above the first phase transition temperature (around 85 °C),
the activation energy was significantly increased because of the thermally
enhanced polaronic effect. Moreover, charge carrier density can be
increased in the D–A nanofibers under visible light illumination.
Consistent with the theoretical models in the literature, the increased
charge carrier density did cause decrease in the activation energy
due to the up-shifting of Fermi level closer to the conduction band
edge