6 research outputs found
Catanionic Surfactant-Assisted Mineralization and Structural Properties of Single-Crystal-like Vaterite Hexagonal Bifrustums
Crystalline vaterite is the most
thermodynamically unstable polymorph of anhydrous calcium carbonate
(CaCO<sub>3</sub>), and various morphologies can be controlled in
the presence of organic additives. Constructing vaterite with minimal
defects, determining its distinctive properties, and understanding
the formation mechanism behind a biomimetic process are the main challenges
in this field. In this paper, a unique single-crystal-like vaterite
hexagonal bifrustum with two hexagonal and 12 trapezoidal faces has
been fabricated through a catanionic surfactant-assisted mineralization
approach for the first time. Compared with the polycrystalline vaterite
aggregates, these bifrustums clearly present a doublet for Raman <i>v</i><sub>1</sub> symmetric stretching mode, a low depolarizaiton
ratio for carbonate molecular symmetry, and a high structural stability.
These indicate a dominant position of hexagonal phase in each crystallite
and confirm the Raman <i>v</i><sub>1</sub> doublet characteristics
of synthetic and biomineral-based vaterites. Our finding may provide
evidence to distinguish vaterite with different structures and shed
light on a possible formation mechanism of vaterite single crystals
Two-Step Freezing in Alkane Monolayers on Colloidal Silica Nanoparticles: From a Stretched-Liquid to an Interface-Frozen State
The
crystallization behavior of an archetypical soft/hard hybrid
nanocomposite, that is, an <i>n-</i>octadecane C<sub>18</sub>/SiO<sub>2</sub>-nanoparticle composite, was investigated by a combination
of differential scanning calorimetry (DSC) and variable-temperature
solid-state <sup>13</sup>C nuclear magnetic resonance (VT solid-state <sup>13</sup>C NMR) as a function of silica nanoparticles loading. Two
latent heat peaks prior to bulk freezing, observed for composites
with high silica loading, indicate that a sizable fraction of C<sub>18</sub> molecules involve two phase transitions unknown from the
bulk C<sub>18</sub>. Combined with the NMR measurements as well as
experiments on alkanes and alkanols at planar amorphous silica surfaces
reported in the literature, this phase behavior can be attributed
to a transition toward a 2D liquid-like monolayer and subsequently
a disorder-to-order transition upon cooling. The second transition
results in the formation of a interface-frozen monolayer of alkane
molecules with their molecular long axis parallel to the nanoparticlesâ
surface normal. Upon heating, the inverse phase sequence was observed,
however, with a sizable thermal hysteresis in accord with the characteristics
of the first-order phase transition. A thermodynamic model considering
a balance of interfacial bonding, chain stretching elasticity, and
entropic effects quantitatively accounts for the observed behavior.
Complementary synchrotron-based wide-angle X-ray diffraction (WAXD)
experiments allow us to document the strong influence of this peculiar
interfacial freezing behavior on the surrounding alkane melts and
in particular the nucleation of a rotator phase absent in the bulk
C<sub>18</sub>
Confined Crystallization of <i>n</i>âHexadecane Located inside Microcapsules or outside Submicrometer Silica Nanospheres: A Comparison Study
Crystallization and phase transition
behaviors of <i>n</i>-hexadecane (<i>n</i>-C<sub>16</sub>H<sub>34</sub>, abbreviated
as C<sub>16</sub>) confined in microcapsules and <i>n</i>-alkane/SiO<sub>2</sub> nanosphere composites have been investigated
by the combination of differential scanning calorimetry (DSC) and
temperature-dependent X-ray diffraction (XRD). As evident from the
DSC measurement, the surface freezing phenomenon of C<sub>16</sub> is enhanced in both the microcapsules and SiO<sub>2</sub> nanosphere
composites because the surface-to-volume ratio is dramatically enlarged
in both kinds of confinement. It is revealed from the XRD results
that the novel solidâsolid phase transition is observed only
in the microencapsulated C<sub>16</sub>, which crystallizes into a
stable triclinic phase via a mestastable rotator phase (RI). For the
C<sub>16</sub>/SiO<sub>2</sub> composite, however, no novel rotator
phase emerges during the cooling process, and C<sub>16</sub> crystallizes
into a stable triclinic phase directly from the liquid state. Heterogeneous
nucleation induced by the surface freezing phase is dominant in the
microencapsulated sample and contributes to the emergence of the novel
rotator phase, whereas heterogeneous nucleation induced by foreign
crystallization nuclei dominates the C<sub>16</sub>/SiO<sub>2</sub> composite, leading to phase transition behaviors similar to those
of bulk C<sub>16</sub>
Unusual Interfacial Freezing Phenomena in Hexacontane/Silica Composites
The
crystallization behaviors of <i>n-</i>hexacontane (C<sub>60</sub>H<sub>122</sub>)/StoÌber silica (SiO<sub>2</sub>) composites
with various compositions were investigated by a combination of differential
scanning calorimetry (DSC), solid-state <sup>13</sup>C nuclear magnetic
resonance (solid-state <sup>13</sup>C NMR), and proton NMR relaxation
experiments. By means of DSC, C<sub>60</sub>H<sub>122</sub> molecules
in C<sub>60</sub>H<sub>122</sub>/silica composites were observed to
be involved in the interfacial freezing not present in the free bulk
C<sub>60</sub>H<sub>122</sub>. The orientation of C<sub>60</sub>H<sub>122</sub> molecules, being preferentially normal to silica surface,
was confirmed by grazing incidence X-ray diffraction experiments on
thin <i>n-</i>hexacontane film adsorbed on the silicon wafer
with a native SiO<sub>2</sub> layer. Inferred from the solid <sup>13</sup>C NMR data, the interfacial monolayer is in orthorhombic
phase with certain chain disorders. It is speculated that the âinterfacial
freezingâ of C<sub>60</sub>H<sub>122</sub> formed in the presence
of silica particles is driven by the combination of the strong attraction
between the molecules and the enhanced number of interfacial molecules
on the silica surface
Oil-in-Water Emulsion Templated and Crystallization-Driven Self-Assembly Formation of Poly(lâlactide)âPolyoxyethyleneâPoly(lâlactide) Fibers
A molecular
solution of an amphiphilic block copolymer may act
as an oil phase by dispersing into an aqueous micellar system of small-molecular
surfactant, forming oil-in-water (O/W) emulsion droplets. In this
paper, an as-synthesized triblock copolymer polyÂ(l-lactide)âpolyoxyethyleneâpolyÂ(l-lactide) (PLLAâPEOâPLLA) was dissolved in tetrahydrofuran
(THF) and then added to an aqueous micellar solution of nonaethylene
glycol monododecyl ether (AEO-9), forming initially coalescent O/W
emulsion droplets in the size range of 35 nmâ1.3 ÎŒm.
Along with gradual volatilization of THF and simultaneous concentration
of PLLAâPEOâPLLA molecules, the amphiphilic copolymer
backbones themselves experience solution-based self-assembly, forming
inverted coreâcorona aggregates within an oil-phase domain.
Anisotropic coalescence of adjacent O/W emulsion droplets occurs,
accompanied by further volatilization of THF. The hydrophilic block
crystallization of core-forming PEOs and the hydrophobic chain stretch
of corona-forming PLLAs together induce the intermediate formation
of rod-like architectures with an average diameter of 300â800
nm, and this leads to a large-scale deposition of the triblock copolymer
fibers with an average diameter of âŒ2.0 ÎŒm. Consequently,
this strategy could be of general interest in the self-assembly formation
of amphiphilic block copolymer fibers and could also provide access
to aqueous solution crystallization of hydrophilic segments of these
copolymers
Controlled Mineralization of Calcium Carbonate on the Surface of Nonpolar Organic Fibers
Isotactic polypropylene (iPP) fiber, the surface of which
is hydrophobic,
can modulate the crystallization polymorphs of calcium carbonate (CaCO<sub>3</sub>) at the air/solution interface under mild conditions. The
present results provide a novel perspective on controlling the crystallization
of biominerals by an insoluble matrix, and they can shed new light
on understanding the biomineralization process of CaCO<sub>3</sub> as it occurs in nature