24 research outputs found
Vanadium Redox Flow Batteries Using <i>meta</i>-Polybenzimidazole-Based Membranes of Different Thicknesses
15,
25, and 35 Ī¼m thick <i>meta</i>-polybenzimidazole
(PBI) membranes are doped with H<sub>2</sub>SO<sub>4</sub> and tested
in a vanadium redox flow battery (VRFB). Their performances are compared
with those of Nafion membranes. Immersed in 2 M H<sub>2</sub>SO<sub>4</sub>, PBI absorbs about 2 mol of H<sub>2</sub>SO<sub>4</sub> per
mole of repeat unit. This results in low conductivity and low voltage
efficiency (VE). In ex-situ tests, <i>meta</i>-PBI shows
a negligible crossover of V<sup>3+</sup> and V<sup>4+</sup> ions,
much lower than that of Nafion. This is due to electrostatic repulsive
forces between vanadium cations and positively charged protonated
PBI backbones, and the molecular sieving effect of PBIās nanosized
pores. It turns out that charge efficiency (CE) of VRFBs using <i>meta</i>-PBI-based membranes is unaffected by or slightly increases
with decreasing membrane thickness. Thick <i>meta</i>-PBI
membranes require about 100 mV larger potentials to achieve the same
charging current as thin <i>meta</i>-PBI membranes. This
additional potential may increase
side reactions or enable more vanadium ions to overcome the electrostatic
energy barrier and to enter the membrane. On this basis, H<sub>2</sub>SO<sub>4</sub>-doped <i>meta</i>-PBI membranes should be
thin to achieve high VE and CE. The energy efficiency of 15 Ī¼m
thick PBI reaches 92%, exceeding that of Nafion 212 and 117 (N212
and N117) at 40 mA cm<sup>ā2</sup>
In Situ Analyses of Carbon Dissolution into Ni-YSZ Anode Materials
A combination of in situ analyses, including measurement
of both
electrical resistance and volumetric expansion, and thermogravimetric
analysis (TGA) was employed to elucidate the deactivation process
of a nickel-yttria-stabilized zirconia (Ni-YSZ) cermet (60 wt % NiO-YSZ)
upon exposure to methane at 750 Ā°C. In conjunction with the aforementioned
in situ techniques, a number of ex situ analyses, including scanning
electron microscopy (SEM), electron probe microanalysis (EPMA), X-ray
diffraction (XRD), and Raman spectroscopy, revealed that carbon deposition
initially occurred at the Ni centers, followed by carbon dissolution
into the Ni-YSZ cermet after an induction period of 200 min, which
then led to three-dimensional expansion. The structural change of
the Ni-based cermet induced increases in electrical resistance of
the material. The increased electrical resistance likely originated
from the breakage of the NiāNi conducting network as well as
from the formation of microscopic cracks within the Ni-YSZ material,
resulting from the observed process of carbon dissolution. Moreover,
a combination of TGA involving measurements of electrical resistance
was demonstrated to be useful for determining amounts of carbon deposits
critical for carbon dissolution. These results strongly suggest that
changes in electrical resistance can be utilized to monitor the extent
of carbon dissolution into the Ni-YSZ catalysts in situ, which would
be helpful for the development of an efficient curing system for solid
oxide fuel cells (SOFCs)
Role of Small Pd Ensembles in Boosting CO Oxidation in AuPd Alloys
We present a theoretical explanation on how PdAu alloy
catalysts
can enhance the oxidation of CO molecules based on density functional
theory calculations of CO adsorption and oxidation on AuPd/Pd(111)
surfaces. Our study suggests that the enhanced activity is largely
attributed to the possible existence of āpartially-poisonedā
Pd ensembles that accommodate fewer CO molecules than Pd atoms. Whereas
the oxidation of preadsorbed CO is likely governed by O<sub>2</sub> trapping, our study shows that small Pd ensembles such as dimers
and compact trimers tend to provide more active sites than larger
ensembles; CO adsorbed on a Pd monomer is found to react hardly with
O<sub>2</sub> to form CO<sub>2</sub>. In addition, we find the tendency
of CO-induced Pd agglomeration, which may in turn facilitate CO oxidation
by creating more dimers and compact trimers as compared with the adsorbate-free
surface where monomers are likely prevailing
Role of Heteronuclear Interactions in Selective H<sub>2</sub> Formation from HCOOH Decomposition on Bimetallic Pd/M (M = Late Transition FCC Metal) Catalysts
In
this study, by using spin-polarized density functional theory
calculations, we have elucidated the role of heteronuclear interactions
in determining the selective H<sub>2</sub> formation from HCOOH decomposition
on bimetallic Pd<sub>shell</sub>/M<sub>core</sub> (M = late transition
FCC metal (Rh, Pt, Ir, Cu, Au, Ag)) catalysts. We found that the catalysis
of HCOOH decomposition strongly depends on the variation of surface
charge polarization (ligand effect) and lattice distance (strain effect),
which are caused by the heteronuclear interactions between surface
Pd and core M atoms. In particular, the contraction of surface PdāPd
bond distance and the increase in electron density in surface Pd atoms
in comparison to the pure Pd case are responsible for the enhancement
of the selectivity to H<sub>2</sub> formation via HCOOH decomposition.
Our calculations also unraveled that the d band center location and
the density of states for the d band (particularly d<sub><i>z</i><sup>2</sup></sub>, d<sub><i>yz</i></sub>, and d<sub><i>xz</i></sub>) near the Fermi level are the important indicators
that explain the impact of strain and ligand effects in catalysis,
respectively. That is, the surface lattice contraction (expansion)
leads to the downshift (upshift) of d band centers in comparison to
the pure Pd case, while the electronic charge increase (decrease)
in surface Pd atoms results in the depletion (augmentation) of the
density of states for d<sub><i>z</i><sup>2</sup></sub>,
d<sub><i>yz</i></sub>, and d<sub><i>xz</i></sub> orbitals. Our study highlights the importance of properly tailoring
the surface lattice distance (d band center) and surface charge polarization
(the density of states for d<sub><i>z</i><sup>2</sup></sub>, d<sub><i>yz</i></sub>, and d<sub><i>xz</i></sub> orbitals near the Fermi level) by tuning the heteronuclear interactions
in bimetallic Pd<sub>shell</sub>/M<sub>core</sub> catalysts for enhancing
the catalysis of HCOOH decomposition toward H<sub>2</sub> production,
as well as other chemical reactions
The miRNA expression profiles were compared between 2D and 3D cultures.
<p>A heatmap of differentially expressed miRNAs generated by unsupervised hierarchical cluster analysis (A). Differential expression levels of miRNAs between 2D and 3D cultures were confirmed using qRT-PCR for several genes selected from microarray data. Among the differentially expressed miRNAs, up-regulated miRNAs including miR-34b-5p, miR-578, miR-1304, and miR-324-5p and down-regulated miRNAs including miR-7-5p, and miR-34b-3p were analyzed using primers for mature mRNAs (B). Data are expressed as the mean Ā± SE of triplicates. * p<0.05, nā=ā3.</p
Analysis of pancreatic cancer stem cell markers.
<p>Expression patterns of stem cell markers such as CD44, CD24, and ESA were compared between 2D (A) and 3D cultures (B). Percentages of the cell population expressing CD44, CD24, and ESA in Panc-1 cells cultured under 2D and 3D conditions are summarized in the table.</p
Differentially expressed miRNAs in Panc-1 cell cultured under 2D and 3D conditions. Fold change indicates 3D intensity/2D intensity.
<p>Differentially expressed miRNAs in Panc-1 cell cultured under 2D and 3D conditions. Fold change indicates 3D intensity/2D intensity.</p
Penetration of DOX into Panc-1 spheroids.
<p>Penetration was evaluated by imaging DOX autofluorescence in sections of spheroids. Spheroids were cultured in a concave microwell 600 plate for 5 Ī¼M for 12 h. Fluorescence intensity across sections was measured and expressed as the mean Ā± SE of 5 replicates. (Scale bar ā=ā100 Ī¼m) * and **, p<0.01 and p<0.001, respectively.</p
Concave PDMS microwell plate for culture and growth of pancreatic tumor spheroids (TS).
<p>Shape and dimension of concave microwell plate 600 (A). Changes in size of three different pancreatic spheroids cultured in microwell 600 (B). Size distribution of Panc-1 spheroids cultured in three different sized-microwell plate during 13 days of culture (C). Data are expressed as mean Ā± SE of a minimum of 10 spheroids cultured in one microwell plate.</p
Morphology and histological examination of tumor spheroids (TS) cultured in concave microwell 600 or in 96 well plates.
<p>Representative images of H&E stained paraffin sections or toluidine blue stained semi-thin sections, SEM and TEM images of HT-29 (A), Panc-1 (B), Aspc-1 (C), and Capan-2 (D) spheroids cultured in concave microwell 600 plates for 5 and 13 days. Aggregates of Panc-1, Aspc-1, and Capan-2 cells formed in agarose-coated 96 well plates shown as an H&E stained paraffin section or bright field images (E). Arrow: desmosome; dotted lines: gap junctions; arrow head: tight junction; cross: lipid droplet; I: invagination structure; N: necrotic regions. The scale bars indicate 100 Ī¼m, 50 Ī¼m, 2 Ī¼m and 500 Ī¼m, in H&E or toluidine blue stained, SEM, TEM and bright-field images, respectively.</p