5 research outputs found
Heterogeneous Photocatalysis and Sensitized Photolysis for Enhanced Degradation of Bisphenol A and its Analogues
This work deals with elucidation of bisphenols transformations occurring in the processes of TiO2 photocatalysis and sensitized photolysis. A special attention is paid to the clarification of the mechanisms of the reactive oxygen species generation. In particular, the work investigates the sources and mobility of photocatalytically generated OH radicals by isotopic labeling experiments and explores the role of natural organic matter as a sensitizer in the sunlight photolysis of bisphenols
Alleviating Anisotropic Volume Variation at Comparable Li Utilization during Cycling of Ni-Rich, Co-Free Layered Oxide Cathode Materials
Charge Transfer-Induced Lattice Collapse in Ni-Rich NCM Cathode Materials during Delithiation
Ni-rich LiNixCoyMnzO2 (NCM) cathode materials have great potential for application in next-generation lithium-ion batteries owing to their high specific capacity. However, they are subjected to severe structural changes upon (de)lithiation, which adversely affects the cycling stability. Herein, we investigate changes in crystal and electronic structure of NCM811 (80% Ni) at high states of charge by a combination of operando X-ray diffraction (XRD), operando hard X-ray absorption spectroscopy (hXAS), ex situ soft X-ray absorption spectroscopy (sXAS), and density functional theory (DFT) calculations, and correlate the results with data from galvanostatic cycling in coin cells. XRD reveals a large decrease in unit cell volume from 101.38(1) Å3 to 94.26(2) Å3 due to collapse of the interlayer spacing when x(Li) < 0.5 (decrease in c-axis from 14.469(1) Å at x(Li) = 0.6 to 13.732(2) Å at x(Li) = 0.25). hXAS shows that the shrinkage of the transition metal-oxygen layer mainly originates from nickel oxidation. sXAS, together with DFT-based Bader charge analysis, indicates that the shrinkage of the interlayer, which is occupied by lithium, is induced by charge transfer between O 2p and partially filled Ni eg orbitals (resulting in decrease of oxygen-oxygen repulsion). Overall, the results demonstrate that high-voltage operation of NCM811 cathodes is inevitably accompanied by charge transfer-induced lattice collapse
Between Scylla and Charybdis: Balancing Among Structural Stability and Energy Density of Layered NCM Cathode Materials for Advanced Lithium-Ion Batteries
Two
major strategies are currently pursued to improve the energy density
of lithium-ion batteries using LiNi<sub><i>x</i></sub>Co<sub><i>y</i></sub>Mn<sub><i>z</i></sub>O<sub>2</sub> (NCM) cathode materials. One is to increase the fraction of redox
active Ni (≥80%), which allows larger amounts of Li to be extracted
at a given cutoff voltage (<i>U</i><sub>max</sub>). The
other is to increase <i>U</i><sub>max</sub>, in particular
for medium-Ni content NCM materials. However, the accompanying lattice
changes ultimately lead to capacity fading in both cases. Here the
structural changes occurring in Li<sub>1.02</sub>Ni<sub><i>x</i></sub>Co<sub><i>y</i></sub>Mn<sub><i>z</i></sub>O<sub>2</sub> (with <i>x</i> = <sup>1</sup>/<sub>3</sub>, 0.5, 0.6, 0.7, 0.8 and 0.85) during cycling operation in the voltage
range between 3.0 and 4.6 V vs Li are quantified by means of <i>operando</i> X-ray diffraction combined with detailed Rietveld
analysis. All samples show a large decrease in unit cell volume upon
charging, ranging from 2.4% for NCM111 (33% Ni) to 8.0% for NCM851005
(85% Ni). To make a fair comparison of the structural stability of
the different NCM materials, energy densities as a function of <i>U</i><sub>max</sub> are estimated and correlated with X-ray
diffraction results. It is shown that NCMs with a lower Ni content
allow for specific energies similar to that of, e.g., Ni-rich NCM811
(80% Ni) when operated at sufficiently high <i>U</i><sub>max</sub>, but still undergo less pronounced changes in structure.
Nevertheless, as indicated by charge/discharge tests, the capacity
retention of low- and medium-Ni content NCMs cycled to high <i>U</i><sub>max</sub> is also strongly affected by factors other
than stability of the layered crystal lattice (electrolyte decomposition
etc.). Overall, it is demonstrated that the complexity of the degradation
processes needs to be better understood to identify optimal cycling
conditions for specific cathode compositions
Anisotropic Lattice Strain and Mechanical Degradation of High- and Low-Nickel NCM Cathode Materials for Li-Ion Batteries
In
the near future, the targets for lithium-ion batteries concerning
specific energy and cost can advantageously be met by introducing
layered LiNi<sub><i>x</i></sub>Co<sub><i>y</i></sub>Mn<sub><i>z</i></sub>O<sub>2</sub> (NCM) cathode
materials with a high Ni content (<i>x</i> ≥ 0.6).
Increasing the Ni content allows for the utilization of more lithium
at a given cell voltage, thereby improving the specific capacity but
at the expense of cycle life. Here, the capacity-fading mechanisms
of both typical low-Ni NCM (<i>x</i> = 0.33, NCM111) and
high-Ni NCM (<i>x</i> = 0.8, NCM811) cathodes are investigated
and compared from crystallographic and microstructural viewpoints.
In situ X-ray diffraction reveals that the unit cells undergo different
volumetric changes of around 1.2 and 5.1% for NCM111 and NCM811, respectively,
when cycled between 3.0 and 4.3 V vs Li/Li<sup>+</sup>. Volume changes
for NCM811 are largest for <i>x</i>(Li) < 0.5 because
of the severe decrease in interlayer lattice parameter <i>c</i> from 14.467(1) to 14.030(1) Å. In agreement, in situ light
microscopy reveals that delithiation leads to different volume contractions
of the secondary particles of (3.3 ± 2.4) and (7.8 ± 1.5)%
for NCM111 and NCM811, respectively. And postmortem cross-sectional
scanning electron microscopy analysis indicates more significant microcracking
in the case of NCM811. Overall, the results establish that the accelerated
aging of NCM811 is related to the disintegration of secondary particles
caused by intergranular fracture, which is driven by mechanical stress
at the interfaces between the primary crystallites