6 research outputs found
Radiative Cooling Face Mask
Radiative cooling is a zero energy
consumption surface cooling
technology, which appears to be a viable option for the development
of radiative cooling face masks. After the COVID-19 pandemic, face
masks have become crucial protective equipment in our daily lives,
protecting from inhalation of fine particulate matter (PM) and also
viruses. However, wearing conventional face masks for a long time
is very unpleasant due to swelter on the face, especially in the outdoor
sunlight environment. In this study, a radiative cooling polymer-based
composite material (PCM) face mask has been designed and demonstrated
experimentally to enhance the wearing comfort of the users including
protection from PM and viruses. With a single layer of the silver
nanoparticle coating, a PCM face mask has high efficiency to block
sunlight by reducing solar transmittance and emit radiation by higher
IR emissivity. Additionally, outdoor measurements with a simulated
skin under the sun was carried out, and the PCM face mask showed a
notable 4 Ā°C cooling impact in comparison to the bare mask
Understanding the Conduction Mechanism of the Protonic Conductor CsH<sub>2</sub>PO<sub>4</sub> by Solid-State NMR Spectroscopy
Local dynamics and hydrogen bonding
in CsH<sub>2</sub>PO<sub>4</sub> have been investigated by <sup>1</sup>H, <sup>2</sup>H, and <sup>31</sup>P solid-state NMR spectroscopy
to help provide a detailed
understanding of proton conduction in the paraelectric phase. Two
distinct environments are observed by <sup>1</sup>H and <sup>2</sup>H NMR, and their chemical shifts (<sup>1</sup>H) and quadrupolar
coupling constants (<sup>2</sup>H) are consistent with one strong
and one slightly weaker H-bonding environment. Two different protonic
motions are detected by variable-temperature <sup>1</sup>H MAS NMR
and <i>T</i><sub>1</sub> spinālattice relaxation
time measurements in the paraelectric phase, which we assign to librational
and long-range translational motions. An activation energy of 0.70
Ā± 0.07 eV is extracted for the latter motion; that of the librational
motion is much lower. <sup>31</sup>P NMR line shapes are measured
under MAS and static conditions, and spinālattice relaxation
time measurements have been performed as a function of temperature.
Although the <sup>31</sup>P line shape is sensitive to the protonic
motion, the reorientation of the phosphate ions does not lead to a
significant change in the <sup>31</sup>P CSA tensor. Rapid protonic
motion and rotation of the phosphate ions is seen in the superprotonic
phase, as probed by the <i>T</i><sub>1</sub> measurements
along with considerable line narrowing of both the <sup>1</sup>H and
the <sup>31</sup>P NMR signals
Revealing Local Dynamics of the Protonic Conductor CsH(PO<sub>3</sub>H) by Solid-State NMR Spectroscopy and First-Principles Calculations
A joint
study incorporating multinuclear solid-state NMR spectroscopy and
first-principles calculations has been performed to investigate the
local structure and dynamics of the protonic conductor CsHĀ(PO<sub>3</sub>H) in the paraelectric phase. The existence of the superprotonic
phase (>137 Ā°C) is clearly confirmed by NMR, in good agreement
with the literature. The variable-temperature <sup>1</sup>H, <sup>2</sup>H, and <sup>31</sup>P NMR data further reveal a distribution
of motional correlation times, with isotropic rotation of the phosphite
ion being observed below the superprotonic phase transition for a
small but gradually increasing subset of anions. This isotropic rotation
is associated with fast local protonic motion, with the distribution
of correlation times being tentatively assigned to internal defects
or surface adsorbed H<sub>2</sub>O. The phosphite ion dynamics of
the majority slower subset of phosphite ions is quantified through
analysis of variable-temperature <sup>17</sup>O spectra recorded from
34 to 150 Ā°C, by considering a model for the pseudo <i>C</i><sub>3</sub> rotation of the phosphite ion around the PāH
bond axis below the phase transformation. An extracted activation
energy of 0.24 Ā± 0.08 eV (23 Ā± 8 kJ mol<sup>ā1</sup>) for this model was obtained, much lower than that reported from
proton conductivity measurements, implying that no strong correlation
exists between long-range protonic motion and <i>C</i><sub>3</sub> rotations of the phosphite. We conclude that proton conduction
in CsHĀ(PO<sub>3</sub>H) in the paraelectric phase is governed by
the activation energy for exchange between donor and acceptor oxygen
sites, rotation of the phosphite units, and the lack of isotropic
rotation of the phosphite ion. Surprisingly, coalescence of <sup>17</sup>O NMR resonances, as would be expected for rapid isotropic reorientations
of all phosphite groups, is not observed above the transition. Potential
reasons for this are discussed
Probing Oxide-Ion Mobility in the Mixed IonicāElectronic Conductor La<sub>2</sub>NiO<sub>4+Ī“</sub> by Solid-State <sup>17</sup>O MAS NMR Spectroscopy
While solid-state NMR spectroscopic
techniques have helped clarify
the local structure and dynamics of ionic conductors, similar studies
of mixed ionicāelectronic conductors (MIECs) have been hampered
by the paramagnetic behavior of these systems. Here we report high-resolution <sup>17</sup>O (<i>I</i> = 5/2) solid-state NMR spectra of the
mixed-conducting solid oxide fuel cell (SOFC) cathode material La<sub>2</sub>NiO<sub>4+Ī“</sub>, a paramagnetic transition-metal oxide.
Three distinct oxygen environments (equatorial, axial, and interstitial)
can be assigned on the basis of hyperfine (Fermi contact) shifts and
quadrupolar nutation behavior, aided by results from periodic DFT
calculations. Distinct structural distortions among the axial sites,
arising from the nonstoichiometric incorporation of interstitial oxygen,
can be resolved by advanced magic angle turning and phase-adjusted
sideband separation (MATPASS) NMR experiments. Finally, variable-temperature
spectra reveal the onset of rapid interstitial oxide motion and exchange
with axial sites at ā¼130 Ā°C, associated with the reported
orthorhombic-to-tetragonal phase transition of La<sub>2</sub>NiO<sub>4+Ī“</sub>. From the variable-temperature spectra, we develop
a model of oxide-ion dynamics on the spectral time scale that accounts
for motional differences of all distinct oxygen sites. Though we treat
La<sub>2</sub>NiO<sub>4+Ī“</sub> as a model system for a combined
paramagnetic <sup>17</sup>O NMR and DFT methodology, the approach
presented herein should prove applicable to MIECs and other functionally
important paramagnetic oxides
Adsorption Behavior of Dyestuffs on Hollow Activated Carbon Fiber from Biomass
<div><p>This study focuses on the adsorption behavior of typical dyestuffs (methylene blue and reactive black 5) on hollow activated carbon fibers (ACFs) obtained from Kapok- and Hasuo-seed based biomass. It was found that the adsorption of dyestuffs on ACFs increased with increasing pH and temperature. In addition, the Hasuo-seed based ACFs showed higher adsorption capacities than the Kapok-seed based ACFs for dyestuffs. It was also determined from the adsorption energy distribution results that the ACFs are having energetically heterogeneous surfaces. The results clearly indicated that the prepared ACF in this study could efficiently remove dyes dissolved in water.</p></div
The Effect of Water on Quinone Redox Mediators in Nonaqueous LiāO<sub>2</sub> Batteries
The parasitic reactions associated
with reduced oxygen species
and the difficulty in achieving the high theoretical capacity have
been major issues plaguing development of practical nonaqueous Li-O<sub>2</sub> batteries. We hereby address the above issues by exploring
the synergistic effect of 2,5-di-<i>tert</i>-butyl-1,4-benzoquinone
and H<sub>2</sub>O on the oxygen chemistry in a nonaqueous Li-O<sub>2</sub> battery. Water stabilizes the quinone monoanion and dianion,
shifting the reduction potentials of the quinone and monoanion to
more positive values (vs Li/Li<sup>+</sup>). When water and the quinone
are used together in a (largely) nonaqueous Li-O<sub>2</sub> battery,
the cell discharge operates via a two-electron oxygen reduction reaction
to form Li<sub>2</sub>O<sub>2</sub>, with the battery discharge voltage,
rate, and capacity all being considerably increased and fewer side
reactions being detected. Li<sub>2</sub>O<sub>2</sub> crystals can
grow up to 30 Ī¼m, more than an order of magnitude larger than
cases with the quinone alone or without any additives, suggesting
that water is essential to promoting a solution dominated process
with the quinone on discharging. The catalytic reduction of O<sub>2</sub> by the quinone monoanion is predominantly responsible for
the attractive features mentioned above. Water stabilizes the quinone
monoanion via hydrogen-bond formation and by coordination of the Li<sup>+</sup> ions, and it also helps increase the solvation, concentration,
lifetime, and diffusion length of reduced oxygen species that dictate
the discharge voltage, rate, and capacity of the battery. When a redox
mediator is also used to aid the charging process, a high-power, high
energy density, rechargeable Li-O<sub>2</sub> battery is obtained