50 research outputs found
Crystallization of Confined Water Pools with Radii Greater Than 1 nm in AOT Reverse Micelles
Freezing of water pools inside aerosol
sodium bisÂ(2-ethylhexyl)
sulfosuccinate (AOT) reverse micelles has been investigated. Previous
freezing experiments suffer from collision and fusion of AOT micelles
and resultant loss of water from the water pool by shedding out during
the cooling process. These phenomena have restricted the formation
of ice to only when the radius of the water pool (<i>R</i><sub>w</sub>) is below 1 nm, and only amorphous ice has been observed.
To overcome the size limitation, a combination of rapid cooling and
a custom-made cell allowing thin sample loading is applied for instantaneous
and homogeneous freezing. The freezing process is monitored with attenuated
total reflection infrared spectroscopy (ATR-IR) measurements. A cooling
rate of ca. −100 K/min and a sample thickness of ca. 50 μm
overcomes the limitations mentioned above and allows the crystallization
of water pools with larger radii (<i>R</i><sub>w</sub> >
1 nm). The corresponding ATR-IR spectra of the frozen water pools
with <i>R</i><sub>w</sub> < 2.0 nm show similar features
to the spectrum of metastable cubic ice (I<sub>c</sub>). Further increase
of the radius of the water pool (<i>R</i><sub>w</sub> >
2.0 nm), unfortunately, drastically decreased the integrated area
of the νÂ(OH) band observed just after freezing, indicating the
breakup of the micellar structure and shedding out of the water pool.
In addition, it was revealed that I<sub>c</sub> ice can also be formed
in flexible organic self-assembled AOT reverse micelles for at least <i>R</i><sub>w</sub> ≤ ca. 2 nm, as well as in inorganic
and solid materials with a pore radius of ca. 2 nm. The dependence
of the phase transition temperature on the curvature of the reverse
micelles is discussed from the viewpoint of the Gibbs–Thomson
effect
Efficient Catalytic Epoxidation in Water by Axial N‑Ligand-Free Mn-Porphyrins within a Micellar Capsule
Epoxidation
of styrenes is efficiently catalyzed by micelle-like
molecular capsules providing Mn-porphyrins in water at room temperature.
In contrast to usual Mn-porphyrin catalysts, the encapsulated Mn-porphyrin
catalysts show higher reactivities (up to 1350 TON for 1 h) even without
the addition of imidazole ligands. Spectroscopic studies and competitive-binding
experiments demonstrate that the efficient catalytic cycle stems from
the enforced proximity of the catalyst and substrates as well as the
smooth replacement of the products by substrates in the hydrophobic
cavity of the capsule
High-Speed Morphology Control of Boehmite Nanoparticles by Supercritical Hydrothermal Treatment with Carboxylic Acids
This
study demonstrates that the morphology of boehmite (AlOOH)
nanoparticles can be controlled over a short timespan by supercritical
hydrothermal treatment in the presence of alkyl carboxylic acids including
hexanoic, octanoic, decanoic, tetradecanoic, and octadecanoic acids.
Boehmite nanoparticles were treated with carboxylic acid in supercritical
water at 400 °C and at a water density of 0.35 g/cm<sup>3</sup> in a batch-type reactor. When the carboxylic acid was not added,
the particles were shaped as rhombic plates. However, the addition
of carboxylic acid changed the crystal morphology to hexagonal plates.
The aspect ratio (i.e., [length along the <i>a</i>-axis]/[length
along the <i>c</i>-axis]) of the rhombic plates increased
with a treatment time of 2–30 min, which is a much shorter
timespan than that used for conventional hydrothermal crystallization.
The aspect ratio of the hexagonal plates increased with increasing
concentration of alkyl carboxylic acids. These results clearly indicate
that carboxylic acids enhance the dissolution and recrystallization
of boehmite. The aspect ratio increased with decreasing length of
the alkyl chain of alkyl-carboxylic acid added to the system. Thermogravimetric
analysis (TGA) showed that carboxylic acids modified the surface of
the boehmite particles. The coverage of the alkyl carboxylic acid
on the surface of the nanoparticles was evaluated from the weight
loss curve obtained from TGA, and the surface area was evaluated from
transmission electron microscopy, which showed that the aspect ratio
of the particles increased with increasing the coverage. The results
suggest that the carboxylic acid suppresses crystal growth along the
shorter axis through surface-capping, thus enhancing dissolution and
crystal growth along the <i>a</i>-axis
Electrical Conductivities, Viscosities, and Densities of <i>N</i>-Methoxymethyl- and <i>N</i>-Butyl-<i>N</i>-methylpyrrolidinium Ionic Liquids with the Bis(fluorosulfonyl)amide Anion
This paper reports the densities, viscosities, and electrical
conductivities
of the two pyrrolidinium ionic liquids, <i>N</i>-methoxymethyl-<i>N</i>-methylpyrrolidinium bisÂ(fluorosulfonyl)Âamide ([Pyr<sub>1,1O1</sub>]Â[FSA]) and <i>N</i>-butyl-<i>N</i>-methylpyrrolidinium bisÂ(fluorosulfonyl)Âamide ([Pyr<sub>1,4</sub>]Â[FSA]), over the temperature range <i>T</i> = (273.15
to 363.15) K at atmospheric pressure. The densities were fitted to
polynominals, and the viscosities and electrical conductivities were
analyzed with the Vogel–Fulcher–Tammann and Litovitz
equations. The densities and electrical conductivities of [Pyr<sub>1,1O1</sub>]Â[FSA] are higher than those of [Pyr<sub>1,4</sub>]Â[FSA],
while the viscosities of the former salt are smaller than those of
the latter. The Walden plots (double logarithm graph of molar conductivity
vs fluidity (reciprocal viscosity)) give the straight lines with the
slopes being 0.91 to 0.94. The present results for [Pyr<sub>1,1O1</sub>]Â[FSA] and [Pyr<sub>1,4</sub>]Â[FSA] are compared with those for the
bisÂ(trifluoromethanesulfonyl)Âamide ([NTf<sub>2</sub>]<sup>−</sup>) analogues, [Pyr<sub>1,1O1</sub>]Â[NTf<sub>2</sub>] and [Pyr<sub>1,4</sub>]Â[NTf<sub>2</sub>]
Attack rate during the influenza A(H3N2) outbreak period.
<p>Attack rate for (A) children aged <20 years and (B) adults aged ≥20 years.</p
Epidemic curves for each affiliation.
<p>Epidemic curves of household transmission index cases, household transmission secondary cases, and non-household transmission ILI cases in (A) school A, (B) school B, (C) preschool C, (D) preschool D, (E) preschool E, (F) preschool F, (G) children at home, and (H) adults. The letters attributed to the household transmission secondary cases are the affiliations of their index cases; A, school A; B, school B; C, preschool C; D, preschool D; E, preschool E; F, preschool F; G, children at home; H, adults.</p
Secondary attack rates and relative risk of ILI by age and gender of household contacts.
<p>Abbreviations: ILI, influenza-like illness; SAR, secondary attack rate; CI, confidence interval; NA, not applicable.</p
Secondary attack rates and relative risk of ILI by household size.
<p>Abbreviations: ILI, influenza-like illness; SAR, secondary attack rate; CI confidence interval.</p
Secondary attack rates and relative risk of ILI by age group of index cases.
<p>Abbreviations: ILI, influenza-like illness; SAR, secondary attack rate; CI, confidence interval; NA, not applicable.</p
Relationship between index cases and secondary cases with household transmission.
<p>Relationship of household transmission (A) among children and (B) among children and adults. Red circles represent index cases, blue triangles represent secondary cases, and arrows show the direction of transmission. The letters represent affiliations; A: school A; B: school B; C: preschool C; D: preschool D; E: preschool E; F: preschool F; G: children at home; H: adults.</p